Nakarin Subjalearndee and
Varol Intasanta*
Nano Functional Textile Laboratory, National Nanotechnology Center, National Science and Technology Development Agency, 111 Phahonyothin Road, Klong Nueng, Klong Luang, Pathumthani 12120, Thailand. E-mail: varol@nanotec.or.th
First published on 22nd August 2016
With unprecedented solar light active ZnWO4/mixed-phased TiO2 nanofibers as a model nanostructure, we showed that by simply allowing as-spun organic–inorganic hybrid samples to undergo thermal relaxation in combination with fiberglass confined calcination, as-desired and free-standing metal oxide nanofibrous membranes could be achieved for the first time. Under an electron microscope, the resulting metal oxide nanofibers were revealed to be freely interwoven without fixed crosslinks between the two contacting points and the fiber’s contour between any two slightly touching points appeared either curved or moderately digressed away from their original direction. The absence of crosslinking was attributed to the porous surface of the fiberglass fabric which offered a certain degree of spatial freedom to the membranes during calcination, leading to enhanced stress relaxation within the fiber during thermal annealing above the materials’ Tg. Such unique fibrous conformations promoted stress transfer along the fibers’ contours and prevented any possible stress concentration, enabling the calcined sample to withstand certain degrees of mechanical stress and so become less likely to fracture. We further demonstrated that the specific combination of metal precursors led to a photocatalytic platform for solar light induced deposition of a single layer of fully dispersed and highly catalytic noble metal nanoparticles.
In recent years, several metal oxide nanostructures have been synthesized in several forms such as nanospheres, nanorods, nanofibers or nanofilms.2,7–9 The nanofibrous form stands out in terms of its uncompromising benefits of chemical versatility and highly accessible surface area due to its zero degree of agglomeration unlike its nanosphere counterpart.10 However, a limited amount of research has been conducted into making these nanofibers into more viable structures to push the potential of this technology beyond laboratory studies towards practicality. The main reason is because metal oxide nanofibers are so fragile that their assembly into nanofibrous membranes can be quite a challenge. Specifically, advances towards thermally and mechanically stable stand-alone metal nanofibrous membranes have been limited by both a lack of understanding of the root causes of fragility and the small number of relevant investigations.
Capable of producing long and continuous fibrous constructs, electrospinning11 is a potential method for the fabrication of stand-alone nanofibrous membranes. For metal oxides, high temperature treatment and crystallization are two interrelated processes which govern the final physical structure, especially crystallinity. Nevertheless, the nanofibers constructed often suffer drastic physical transformations, extreme fragility and break down into short fibers immediately after calcination. The same is true for several high activity and low environmental and health impact photocatalysts derived from metal oxides such as tungsten oxide (WO3),12 titanium dioxide (TiO2)13 and zinc oxide (ZnO).14 Specifically, active towards visible, UV and solar light, these materials show benefits for applications in sensing, catalysis and electrochromics.14–17
While the broad compositional possibilities among metal oxides have been considered endless, the incorporation of metals could be a prerequisite for several advancements.3,18,19 In particular, metal/metal oxide hybrid materials have emerged as potential hybrid materials for a broad range of applications, especially in environmental and energy applications.8,20–23
Among the greatest global challenges, environmental issues are the subject that can be dealt with effectively by photocatalysis. Clean air and water have become both societal and economic challenges affecting the wellbeing of people from all walks of life. Considered as state-of-the-art advances for water remediation, filtration,11,24 absorption25,26 and sedimentation27–29 are applicable for colloids and solid suspensions. However, their limitation leaves quite a large performance gap for chemical and biological contaminants, the two major classes of waste water from industrial production plants, hospitals and scientific laboratories, etc. These two types of injurious pollutants require specially designed catalyts.30
In this present contribution, with Pd/Pt-decorated solar light active ZnWO4/mixed-phased TiO2 nanofibers as a model subject, we investigate three aspects as prerequisites for the construction of mechanically stable metal oxide nanofibrous membranes. These involve (i) the processing of organic–inorganic nanofiber fabrications by electrospinning, (ii) the thermal transformation of the hybrid nanofibers and most importantly (iii) probing the physical structures of the resulting all-inorganic nanofibrous membranes. During our investigations, we analyse the point at which the presence of a single-crystal induced void manifests into a determining structural factor that affects the nanofibers’ physical stability. In addition, we study the correlation between the spatial distribution among the resulting all-inorganic nanofibers and the fragility at the membrane level. Following the stability improvements, we further demonstrate that the unique combination of nanofiber metal oxides leads to a photocatalytic platform for further light-induced noble metal nanoparticle deposition. Interestingly, the deposited metal forms a single layer of fully dispersed and supported metal nanoparticles making the hybrids advantageous for catalysis and sensing for energy and environmental applications that particularly require comprehensive accessibility to the catalytic active sites.
300
000, Fluka), palladium(II) nitrate hydrate (Pd(NO3)2·xH2O, Sigma Aldrich), chloroplatinic acid hexahydrate (H2PtCl6·6H2O, Sigma Aldrich) and glacial acetic acid (Sigma Aldrich), were of analytical grade and used as received.
The crystal structures of the metal oxide nanofibers were determined from X-ray diffraction (XRD) patterns in a range of 2θ = 15–80° using an X-ray diffractometer (Bruker, D8 advance) with a Cu source (λ = 1.542 Å).
Quantification of gas elimination was performed using gas chromatography/mass spectrometry (GC/MS 5975, Agilent Capillary Column DB-624 60 m, 0.25 mm 1.40 S/N, USA. Network headspace sampler (G 1888)).
For the photodeposition under solar light, a similar suspension was prepared. The nanofibrous membrane (50 mg) was suspended in DI water (60 ml). Then, palladium(II) nitrate hydrate (1 mg) and chloroplatinic acid hexahydrate (3 mg) were added into the solution and magnetically stirred for an hour under natural sunlight. Finally, the resulting yellowish suspension was filtered, washed and dried at 60 °C for an hour.
000 rpm for 10 minutes) and filtered to remove the photocatalyst. Subsequently, the concentration of MB was measured using a UV-Vis spectrophotometer (Perkin Elmer, Lambda 650, USA) at 663 nm, the maximum absorption of MB. After the first catalytic cycle, the remaining suspension was centrifuged at 10
000 rpm for 10 minutes. Then, the MB solution was separated from the catalyst which was subsequently rinsed and dried at room temperature for an hour. Catalytic reactions using the MB solution were performed until five cycles were complete.
In the following experiment, P25 was replaced by TIP as an alternative precursor for the UV light active component. However, this resulted in an opaque solution. Such an observation could be explained by the condensation of TIP which was caused by the surrounding moisture favoring formation of minute solid particles suspended throughout the solution. However, subsequent nanofiber fabrication using the Nanospider machine resulted in large diameter and non-homogeneous fibers (Fig. S1e, ESI†). After calcination at 500 °C, clusters of particles appeared in the absence of fiber formation as one would expect (Fig. S1f, ESI†).
In order to avoid the self-condensation of TIP in such moisture containing environments, organic solvents became the media of interest. However, complete elimination of water would result in a suspension of ZAH due to its insolubility in the remaining ethanol. As a consequence, DMF was introduced to replace the water content of the solution mixtures. After mixing ZAH with the rest of the precursors, the resulting solution appeared clear, homogeneous and yellowish with no trace of solid particulates from TIP condensates as observed previously. The following electrospun nanofibers were homogeneous in shape and size (Fig. S2a, ESI†). After calcination at 500 °C, well-defined nanofibers were obtained with a slight reduction in the fibers’ diameter due to the elimination of the original carbon-containing constituents (Fig. S2b, ESI†).
Typically, the degree of heat treatment strongly influenced the crystal structure and final properties of the metal oxides. In order to investigate the relevance of this influence, three variations of calcination temperatures were performed at 500, 600, and 700 °C. Interesting morphological changes on the nanofibers’ surface were observed after calcination at 600 °C (Fig. 1a), with rod-like nanostructures stemming from the surface along the nanofibers. Similar surface distortions were also discerned for a sample treated at 700 °C (Fig. S2d, ESI†). Under SEM-EDX, all characteristic elemental footprints, Zn, W, and Ti, were found in the absence of carbon content (Fig. S3, ESI†).
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| Fig. 1 (a) SEM image of nanofibers after calcination at 600 °C. (b) HRTEM of (a). (c–e) HRTEM of selected areas in (b). (f) Nanorod on the nanofiber. (g) HRTEM of (f). | ||
The effect of thermal treatment was further rationalized at the crystal structure level. X-ray diffraction (XRD) patterns of the metal oxide nanofibers from three varying calcination temperatures are illustrated in Fig. S4 (ESI†). In the absence of zinc oxide or tungsten oxide diffraction footprints, only a TiO2 anatase crystalline structure formed in the nanofibers after calcination at 500 °C. At the higher calcination temperature (600 °C), both characteristic crystalline structures of TiO2, anatase and rutile, were distinguished as major phases, with ZnWO4 in a sanmatinite crystalline structure32 as a minor phase. At the highest calcination temperature (700 °C), clear characteristic peaks of sanmatinite phase ZnWO4 were still discernable while the rutile phase of TiO2 dominated over the anatase phase. From FWHM (full width at half maximum), the average anatase crystalline size of TiO2 after calcination at 500, 600, and 700 °C was 11.5, 13.7, and 40.4 nanometers, respectively. The increase in crystal size was hypothesized to be due to the higher energy given to the samples at higher temperatures to have their bulk reach structural equilibrium.
The morphology of the metal oxide nanofibers was further demonstrated by TEM. Under a scanning and transmission mode, all three crystalline domains of TiO2 and ZnWO4 were observed using HRTEM (Fig. 1b) and SAED measurements (Fig. S5, ESI†). Fig. 1c illustrates the diffraction spacing of the (011) planes of ZnWO4 while Fig. 1d and e shows the diffraction spacing of the (004) planes of anatase and the (101) planes of rutile crystal structures of TiO2, respectively. In addition, TEM-EDX confirmed the presence of the three key elements, Ti, Zn and W, as expected from such a triple metal composite (Fig. S5f, ESI†).
The uniquely present rod-like structures were also scrutinized using HRTEM. It was primarily observed that the minute structure embodied a well-defined rod shape with a persistent diameter of 60 nanometers, stemming almost vertically from the fiber’s surface (Fig. 1f). To elaborate on the crystallographic structure of the nanorod, SAED measurements (Fig. 1f inset) and HRTEM (Fig. 1g) helped identify the interplanar spacings of the lattice fringes. The result suggested that these nanorods conveyed a diffraction spacing that belonged to the (121) planes of ZnWO4, confirming the existence of ZnWO4/mixed-phased TiO2 nanofibers as an output. Interestingly, under the TEM-EDX mode, it was unveiled that titanium took no part in the chemical composition of those nanorods (Fig. S6f, ESI†). However, to the best of our knowledge, this was the first time that nanorods could be grown from the surface of metal oxide nanofibers via a single step electrospinning process and subsequent thermal treatment. From the above crystal developments, it was hypothesized that phase separations among the emerging stable and distinctive single crystals could be a driving force behind the formation of these nanorods at the surface. Consequently, in-depth characterization of ZnWO4/mixed-phased TiO2 nanofibers was further carried out using XANES (X-ray absorption near edge structure).33–35 In the vicinity of the Zn K-edge (9659 eV), the measurement was completed under fluorescence mode by using a Ge (220) monochromator at BL-5 of the Synchrotron Light Research Institute (SLRI). Fig. 2a shows the XANES spectra of the electrospun nanofibers before and after calcination at three various temperatures compared with Zn foil and ZnO references. Typically, the edge energy positions shifted to a higher level when the oxidation state of the metal ions increased. It could be clearly seen that all the edge energies of all the ZnWO4/mixed-phased TiO2 samples (Fig. 2a(i)) were located close to that of the ZnO reference, insinuating the existence of Zn2+. In addition, the adsorption intensity or white line position (Fig. 2a(ii)) of all the samples gradually increased in unison with the increase of the calcination temperature. This phenomenon is strongly associated with the growth of ZnWO4 crystal size at higher calcination temperatures. Then, it could be said that the change in white line intensity might be influenced by the increase of the crystal sizes. The results above suggested that the existence of Zn2+ persisted during the physical transformation from solution to electrospun nanofibers to metal oxide nanofibers. Therefore, it could be inferred from these results that metal oxides had emerged in the initial state. As the same types of the metal oxide persisted during thermal evolution, phase separations among the emerging stable and distinctive single crystals became a dominant mechanism behind the formation of the nanorods.
Furthermore, the unusual dimensional stability of the resultant ZnWO4/mixed-phased TiO2 nanofibers inspired an in depth investigation of the nanofibers’ structure to determine the physical origin of their physical integrity. In the following structural analysis, brittle WO3 nanofibers were employed as references. Their physical appearance at the nanometer length scale was closely inspected and compared with that of the ZnWO4/mixed-phased TiO2 nanofibers. Under TEM transmission mode, the WO3 nanostructures held a low degree of structural homogeneity, as fully developed single crystals were predominant (Fig. 2b). A stark contrast was observed for the well-defined nanofibrous structure of the ZnWO4/mixed-phased TiO2 composite which showed densely packed bulk areas along its secure arrangement (Fig. 2c). This could be confirmed using HRTEM of both structures as the WO3 nanofibers are unmistakably composed of loosely packed single crystal building blocks. Such rough nanodomains were completely absent in the firm ZnWO4/mixed-phased TiO2 nanofibers.
Nevertheless, the resultant metal oxide nanofibrous membranes showed a discernable degree of physical surface irregularities that could impede future high quality device fabrications. Thus, we investigated the factors pertinent to structural control towards well-defined metal oxide nanofibrous membranes. First, it was argued that the spatially unconfined electrospun sample thermally and freely transformed into nanofibrous metal oxide membranes with random dimensional evolution. It was then hypothesized that physical confinement could counteract the undesirable physical distortion.
In a subsequent experiment, three identical and physically well-defined electrospun nanofibrous membranes were subjected to high temperature treatment under different degrees of confinement. The first sample was annealed and calcined while sandwiched between two glass slides. Sandwiched between two pieces of fiberglass fabric, the second sample was annealed at 100 °C and calcined at 600 °C, while the third was annealed at 200 °C and calcined at 600 °C.
Under high temperature treatment between glass slides, the calcined nanofibrous membrane retained its flat structure with a smooth surface (Fig. 3e). However, the sample became so fragile and unstable that picking it up using tweezers was found to be impossible as it would readily dissemble into small pieces. In contrast, the other two samples that were thermally treated between two pieces of fiberglass fabric at 100 °C/600 °C (Fig. 3f) and 200 °C/600 °C (Fig. 3g) appeared physically stable with relatively rougher surfaces. It was interesting to note that, for these two samples, thermal treatment caused a 70% reduction in the membranes’ area (Fig. S7 and S8, ESI†). This dimensional shrinkage could be informative during the future planning of such membrane production. Therefore, it could be said that the confinement method during thermal treatment played an influential role on the stability of the final metal oxide nanofibrous membranes.
It was then hypothesized that the form of confinement during the thermal transformation imparted an effect on the structure of the membrane. Consequently, more intriguing characteristics of the thermally treated sandwiched samples were discovered after careful inspection at the nanometer scale as shown in Fig. 4a–d. While the two samples appeared almost identical in terms of the fibers’ characteristic size, shape and degree of surface homogeneity, there was one distinct difference. That was the way the metal oxide nanofibers in the two samples intermingled differently.
For samples from the glass slide sandwiches, the nanofibers were interwoven with physical crosslinks between any two contacting points. It was also observed that the fiber’s contour between these physical crosslinks appeared straight (Fig. 4a and b). It was believed that these crosslinks might have been forced to form because of the rigid and flat surface of the glass slide that introduced absolute spatial confinement to the membranes during and after the calcination. As a consequence, it could be said that such confinement led to reduced stress relaxation in the fiber during annealing at temperatures above the materials’ Tg, forcing the fibers to make contact with each other and finally coalesce. Furthermore, physical crosslinking within the resulting metal oxide nanofibers might have prevented stress transfer along the fibers’ contour that led to stress concentration, making the sample prone to breakage with only slight mechanical perturbation.
Different nanostructures were identified for the metal oxide samples from the fiberglass fabric sandwich. Evidently, the nanofibers were freely interwoven without fixed crosslinks between two contacting points (Fig. 4c and d). Furthermore, the fiber’s contour between any two slightly touching points appeared either curved or moderately digressed away from their original direction. It was hypothesized that the absence of crosslinking could be attributed to the porous surface of the fiberglass fabric which offered a certain degree of spatial freedom to the membranes during the calcination. Arguably, such spatial freedom led to enhanced stress relaxation in the fiber during thermal annealing above the materials’ Tg. Moreover, the looser structure promoted stress transfer along the fibers’ contour and prevented stress concentration, enabling the calcined sample to withstand certain degrees of mechanical stress and so become less likely to fracture.
From the above structure–property understanding, more stable metal oxide nanofibrous membranes could be made into different shapes. For example, we attempted to study the structure of metal oxide nanofibrous membranes under fiberglass sandwich confinement that had been manipulated into various 3D structures. It was noted that such nonconventional conformations might open up new possibilities in future smart device fabrication. The nanofibrous membrane was first sandwiched between two pieces of fiberglass fabric and then put in a beaker prior to high temperature treatment (Fig. S7m, ESI†). It was found that the resultant shape-controlled membrane was not only stable but also slightly flexible in the original bent shape (Fig. 4e). Even more complex metal oxide nanofibrous membrane structures could be successfully created by the same thermal processes but with different supporting sandwich architectures. Fig. S7o (ESI†) showed a membrane before calcination sandwiched between two wavy-shaped pieces of fiberglass fabric. After the calcination, the sample was not only able to maintain its nanofibrous membrane structure but also retained its original wavy shape with high stability and slight flexibility (Fig. 4f). To the best of our knowledge, these observations of thermally and mechanically free-standing metal oxide nanofibrous membranes have never been reported before. It could be said that this novel and yet simple fabrication of stable and flexible 3D metal oxide nanofibrous membranes was a promising step towards overcoming the most crucial drawback of metal oxide membranes, i.e. fragility, which has impeded the scaling up process towards an industrial scale. (The SEM images of nanofibers from each AC process are provided in Fig. S8, ESI†). Various applications such as nanofiltration and flow-through catalytic systems can take advantage of these as-designed and stand-alone membrane designs to fulfil demands previously unmet by their powder counterparts.
Experimentally, photodeposition of Pd and Pt onto the metal oxide nanofibrous membranes was performed under visible, UV and natural sunlight. The resulting metal/metal oxide hybrid materials after photodeposition of the two metals under laboratory generated visible and UV light irradiation were characterized using SEM-EDX, where the presence of the key elements, Pd and Pt, was confirmed (Fig. S9, ESI†). From SEM, it was ascertained that the nanofibrous membrane structures remained intact after the photodeposition reactions (Fig. S10, ESI†). Careful inspection unveiled small dots decorating the surface of the nanofibers. HRTEM further confirmed that these were metal nanoparticles that were also deposited on the ZnWO4 nanorods by photodeposition under visible and UV light irradiation (Fig. S10, ESI†).
After successful photodeposition under laboratory generated visible and UV light, a similar reaction was performed under natural sunlight of 85
300 Lux in intensity (Fig. S11, ESI†). As a consequence, the resulting hybrid materials retained their nanofibrous structure with small rods adhering to the surface (Fig. 5a). Using SEM-EDX, it was found that all three of the above samples contained elemental footprints for both Pd and Pt, confirming successful deposition of the two noble metals (Fig. 5b).
The TEM and HRTEM images, and SAED patterns (Fig. 5c–h) revealed nanosized particles with an average diameter of less than 7 nm attached to the surface of the main fiber and the stemming ZnWO4 nanorods. The interplanar spacing of the round-shaped particles on the surface of the ZnWO4 nanorod was found to be 0.223 and 0.227 nm, corresponding to the (111) crystal planes of Pd and Pt, respectively.
The second photocatalytic performance evaluation involved a demonstrative application of water treatment where ZnWO4/mixed-phased TiO2 nanofibers and Pd/Pt-decorated ZnWO4/mixed-phased TiO2 nanofibers were examined through degradation of methylene blue (MB) in the aqueous phase with WO3 nanofibers as a reference (Fig. 7). The experiment was performed on a sunny day with a clear sky where the sunlight intensity was measured to be close to 83
000 Lux. The three catalysts showed different degradation rates with sunlight exposure. All catalysts showed their highest rates at 15 minutes after starting the reaction, with WO3 nanofibers showing a much lower performance throughout the 6 hours of irradiation time. It was clearly shown that both types of newly developed hybrid nanofibers performed far better than the reference materials, with Pd/Pt-decorated ZnWO4/mixed-phased TiO2 nanofibers showing the most impressive result.
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| Fig. 7 Photocatalytic degradation of MB under sunlight by WO3, ZnWO4/mixed-phased TiO2, and Pd/Pt–ZnWO4/mixed-phased TiO2 nanofibers. (Inset) Experimental set up under natural sunlight. | ||
The third evaluation approach represented a demonstrative application of the catalyst in air treatment via degradation of a benzene/methanol mixture in the gas phase. Due to the high risk associated with the model pollutants, the catalytic degradation was conducted under laboratory-generated visible light with WO3 nanofibers as a reference. Visible light was selected over UV light because it represents 95% of natural solar light.
The three catalysts showed different degradation rates under visible light irradiation (Fig. 8). For air treatment of the two gases, it was found that WO3 nanofibers did not show any activity. In contrast, ZnWO4/mixed-phased TiO2 nanofibers showed a 43% degradation efficiency against 500 ppm benzene. Even though Pd/Pt-decorated ZnWO4/mixed-phased TiO2 nanofibers showed a lower benzene degradation efficiency, they could transform methanol into methyl formate at room temperature.
The results from these model tests suggested that the metal oxide nanofibers could be effective as photocatalysts under visible light for stable air pollutants such as benzene. Moreover, they could also act as a platform for further metal decoration via a facile photodeposition method utilizing their photocatalytic features. The resulting metal/metal oxide hybrids could not only hold the original well-defined nanofibrous membrane, but also offer a versatile catalytic substrate for endless chemical reactions.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c6ra15086a |
| This journal is © The Royal Society of Chemistry 2016 |