Open Access Article
Frances L. Heale
,
Maud Einhorn,
Kristopher Page,
Ivan P. Parkin
and
Claire J. Carmalt
*
Department of Chemistry, University College London, 20 Gordon Street, London, WC1H 0AJ, UK. E-mail: c.j.carmalt@ucl.ac.uk; Tel: +44 (0)20 7679 7528
First published on 28th June 2019
Surfaces that have unique wettabilities and are simultaneously superhydrophobic with water contact angles > 150°, and superoleophilic with oil contact angles < 5°, are of critical importance in the oil/solvent–water separation field. This work details the facile preparation of highly efficient oil–water separation devices that successfully combine hierarchical surface roughening particles and low surface energy components with porous substrates. Coatings were generated using TiO2 and hydrophobic-SiO2 micro/nanoparticle loadings which were then embedded within polydimethylsiloxane, commercially known as Sylgard® 184, and 1H,1H,2H,2H-perfluorooctyltriethoxysilane (FAS) polymer mixtures. The resulting slurries were dip coated onto copper meshes with varying pore diameters (30, 60 and 100 meshes had 595, 250 and 149 μm pore dimensions respectively). Functional testing proved that mesh substrates coated in the lowest Sylgard® 184
:
FAS polymer ratio formulations displayed heightened water repellency and retained their superoleophilic properties upon repeat testing. The largest average water contact angle of 145 ± 1°, was recorded on a copper 30 mesh substrate with a coating comprising H-SiO2 microparticles and TiO2 nanoparticles in a 1
:
9 polymer mixture of Sylgard® and FAS. The coating's extreme oil affinity was supported by high solvent–water separation efficiencies (≥99%) which withstood numerous testing/washing cycles.
000 tonnes of petrochemical oil spilt in aquatic environments, 80% of this amount was lost in just ten incidents.3 It is therefore of great importance to engineer efficient oil–water separation techniques capable of rapidly cleaning the environment in the event of future spills and to decontaminate oily industrial waste.
Interactions between liquids and surfaces are central to this field of research. Superhydrophobic materials often make use of nano and/or microscale protrusions combined with very low surface energy modifications to achieve static water contact angles ≥ 150°.4,5 Water droplets upon these materials can exist in a Wenzel state, whereby the droplets ‘stick’ to all parts of the surface, or Cassie–Baxter regime where droplets ‘slip’ on a lubricating air layer trapped within surface asperities.6,7 The literature details various ways of fabricating novel water repellent surfaces inspired by nature's waterproof materials such as lotus leaves butterfly wings and geckos' feet.5 Plasma enhanced chemical vapor deposition (PECVD) was carried out by Bico et al. to generate carbon flake-like multiscale surface structures.8 Aerosol-assisted chemical vapour deposition (AACVD) of Sylgard® 184 or polydimethylsiloxane (PDMS) and tetraethyl orthosilicate (TEOS) afforded appropriately rough and transparent coatings on glass substrates.9–11 Alternative superhydrophobic generating methods such as chemical etching,12 electrospinning13,14 and lithographic imprinting/templatation15 have enhanced the functionality of oil–water separation, self-cleaning, anti-icing and anti-corrosion materials.12,16–18
Whilst water repellency is crucial to certain oil–water separation devices, materials with two wettability regimes have been known to improve separation efficiency. A surface displaying both superhydrophobic ‘water-hating’ and superoleophilic ‘oil-loving’ properties can be tuned for selective separation providing its surface energy resides between that of the solvent/oil and water it aims to separate (approximately between 30 mN m−1 and 70 mN m−1).19 Filtration and/or absorption are successful types of oil-removing techniques that encompass both size exclusion and wettability selectivity mechanisms. Pore sizes are commonly designed to either let oil run straight through the mesh/membrane or for the material to absorb the hydrocarbon whilst water is repelled.20
Copper meshes have been etched with nitric acid and alkali (NaOH/K2S2O8) solutions before modification with self-assembled monolayers of hexadecanethiol and dodecanethiol respectively. High water contact angles, ∼150°, and low oil contact angles, <5°, produced materials that separated at least 97% of water from an oily solution.21,22 Vertically-aligned multi-walled carbon nanotubes were synthesised on a stainless steel mesh via CVD. Needle-likes tubes created a high surface area and aided capillary action; the oil contact angle was recorded at 0° and oil penetrated the mesh in 0.4 s.23 Li et al. fabricated candle soot and silica coated meshes that repelled hot water and corrosive liquids. These coated meshes worked as effective gravity separation devices with ∼99% of organic solvents permeating through the device.24 Nano protrusions have also been introduced by electrochemical etching, a copper mesh was anodized in a NaOH solution (1 M) to create a needle-like Cu(OH)2 film. The roughened substrate was then coated in a self-assembled monolayer of 1H,1H,2H,2H-perfluorooctyltriethoxysilane (FAS) to form a durable solvent/water separator.25 Spin coating metal mesh substrates with ZnO nanorods has been yet another effective fabrication method.26
Swapping a porous substrate for porous structures (on special materials) enhances robustness by removing the possibility for coating stripping. Tu et al. designed a micro-bead and nanofiber film created in one step by spraying onto any given substrate. The water contact angle on these surfaces was not as high as other but the cost and fabrication time were drastically reduced.27 A thermoplastic polyurethane mat, created via electrospinning, immersed in a hexadecyltrimethoxysilane (HDTMS) modified nanosilica solution also generated an efficient structured separation material.28 Several other surface modification methods such as electrostatic deposition, grafting polymerisation, spray drying and photo-initiated polymerisation have gained traction by utilising various polymers, gels and biomaterials.29,30
Herein we present an extremely facile one-pot method to fabricate highly efficient oil–water separation devices, >99% efficiency. Combinations of hierarchical surface roughening particles and low surface energy components upon porous substrates lead to enhanced robustness and functionality when tested with a variety of common industrial solvents; this elevated device effectiveness across a substrate and solvent range has substantially advanced work in this area. Here, TiO2 and hydrophobic-SiO2 micro/nanoparticles were embedded within polydimethylsiloxane (Sylgard® 184) and 1H,1H,2H,2H-perfluorooctyltriethoxysilane (FAS) polymer mixtures. Resulting slurries were dip coated onto copper meshes with varying pore diameters (30, 60 and 100 meshes had 595, 250 and 149 μm pore dimensions respectively). Water contact angles, solvent separation efficiencies and mechanical stability were found to outperform many of the existing optimum superhydrophobic/superoleophilic filtration surface previously documented.
:
10 mass ratio (30.00 g combined mass) were dissolved in ethanol (150.00 g), Fig. 1a. The polydimethylsiloxane polymer was magnetically stirred for 2 hours. A colourless, viscous mixture was achieved.
![]() | ||
| Fig. 1 Structure of (a) Sylgard® 184 polymer and (b) 1H,1H,2H,2H-perfluorooctyltriethoxysilane prior to polymerisation. | ||
A 1H,1H,2H,2H-perfluorooctyltriethoxysilane (FAS) solution was prepared by magnetically stirring FAS (1.00 g) in ethanol (99.00 g) for 2 hours to produce a clear/colourless solution, Fig. 1b.
For ease of reference the following particle combinations and loadings (embedded in a polymer mixture) have been abbreviated, Table 1. Optimised functional coatings have also been labelled, Table 2.
| Coating label | Particle loading/g | ||
|---|---|---|---|
| TiO2 | H-SiO2 5–15 μm | ||
| 21 nm | 60–200 nm | ||
| A | 0.6 | — | 0.6 |
| B | 0.6 | — | 0.6 |
| C | 1.5 | 1.5 | — |
| Coating label | Particle loading/g | Mixture of polymer stock solutions/g | Sylgard® 184 : FAS ratio |
|||
|---|---|---|---|---|---|---|
| TiO2 | H-SiO2 5–15 μm | Sylgard® 184 | FAS | |||
| 21 nm | 60–200 nm | |||||
| D | 0.6 | — | 0.6 | 3 | 27 | 1 : 9 |
| E | 0.6 | — | 0.6 | 30 | — | 0 : 1 |
| F | 1.5 | 1.5 | — | 6 | 24 | 1 : 4 |
| G | 0.6 | — | 0.6 | 6 | 24 | 1 : 4 |
According to the experimental setup in Fig. 2, solvent–water separation efficiencies were carried out by rapidly pouring oily mixtures over the selected separation device and recording the mass of solvent collected after 30 s (later converted to a percentage of the total solvent content to be separated). Three repeat readings were recorded per separation solution and the initial solvent mass present in the 10 mL mixture was known. One part solvent three parts water (25%), solvent and water in equal parts (50%) and three parts solvent one part water (75%) mixtures of toluene–methylene blue water, hexane–methylene blue water and dichloromethane–methylene blue water (total volume, 10 mL) were the chosen testing solutions.
Meshes were washed with ethanol (5 mL) before and after same solvent separations and new functional meshes were used when solvents were interchanged. Methylene blue water was utilised to prove no water had permeated through the separation mesh as the blue coloured water was easily distinguished from the colourless solvent. Sample durability was further assessed using the Scotch tape test and acid and base baths: Scotch tape was firmly applied to cover the whole sample surface and then ripped/removed at speed 3 times.
:
9 polymer mixture of Sylgard® 184 and FAS, the Si 2p peak was deconvoluted into a 104.00 eV Si–O2 and a 101.82 eV Si–OR environment. Values agreed with the literature and were consistent with other TiO2 and SiO2 particle containing samples.31–34
The X-ray diffraction pattern of coating D displays a high intensity TiO2 anatase peak at 25.4° and subsequently less intense peaks at 36.7°, 37.8°, 38.8°, 47.9°, 54.6°, 55.1° and 62.5°. A medium intensity rutile peak was identified at 27.4° and SiO2 particles were attributed to the quartz peak at 20.8°. As coating F was absent of SiO2 particles the only detectable peaks were characteristic of the anatase and rutile phases of TiO2. All coating patterns presented in Fig. S1† agreed with particle standards and the Inorganic Crystal Structure Database.
Fourier transform infrared (FT-IR) analysis, consistent with the NIST Standard Reference Database, resulted in the identification of several bending and stretching modes characteristic of the Sylgard® 184 and 1H,1H,2H,2H-perfluorooctyltriethoxysilane (FAS) polymer mixtures, Fig. 4. Samples containing hydrophobic-SiO2 (H-SiO2) and/or TiO2 particles embedded in 1
:
0, 0
:
1, 1
:
1, 1
:
4 and 1
:
9 Sylgard® 184
:
FAS ratios all had similar polymer transmittance bands. A sharp peak at 3120 cm−1 was seen in the spectra of coatings D, E, F and G which depicted the C–H alkane stretch present in both polymers. Varying intensities of the following peaks were observed: 1257 cm−1 (sh, w) intense out of phase vinyl ether stretch in Sylgard® 184,35 1010 cm−1 (s) Si–OR Sylgard® 184 and FAS stretch, 790 cm−1 (m) alkene out of plane bending in Sylgard® 184, 622 cm−1 (w) C–F FAS stretch and 457 cm−1 (w) antisymmetric Si–(CH3) Sylgard® 184 stretch.35 The presence of these C–F FAS stretches were synonymous with functional effectiveness; fluorine's extreme electronegativity made it only weakly susceptible to fleeting dipoles that form the basis of van der Waals forces. Consequently, the samples' fluorinated carbon chains had small intermolecular forces and therefore the low surface energy hydrophobic requirement.
![]() | ||
Fig. 4 Fourier transform infrared (FT-IR) spectrum of coating D; SiO2 5–15 μm particles (0.6 g) and TiO2 21 nm particles (0.6 g) in a 1 : 9 polymer mixture of Sylgard® 184 and FAS. | ||
Scanning electron microscopy (SEM) images provided visual information about the topography of separation materials, particle size/distribution and the extent of copper mesh substrate pore blockage. This qualitative evidence was attributed to water contact angle measurements as well as separation efficiency results. Initial trial coatings containing TiO2 particles in high ratios of Sylgard® 184 to FAS (1
:
1 or 1
:
0) resulted in almost complete pore blockage, Fig. S2.† As expected, pore obstruction physically impeded the passage of any solvent through the membrane and resulted in poor separation efficiencies < 25%. Coatings with higher proportions of the more viscous Sylgard® 184 polymer were also seen to reduce the prominence of particle roughening structures thus had reduced average water contact angle values, <110°.
Fig. 5a presents SEM images of the unobstructed pores of a 30 mesh (595 μm pore dimension) copper substrate functionalised with coating D (SiO2 5–15 μm particles (0.6 g) with TiO2 21 nm particles (0.6 g) in a 1
:
9 polymer mixture of Sylgard® 184 and FAS). Dual scale surface structures were accentuated in this coating due to the reduced quantity of Sylgard® 184 and were reflected in the high average water contact angle, 145 ± 1°. However, solvent–water separation testing indicated that the pores were too large to selectively filter solvents from water and so the use of copper 30 mesh substrates were discontinued. Fig. 5b displays a section of coating D adhered to a copper 60 mesh substrate (250 μm pore dimension). Once again, imaging proved that pore openings were clear. The average water contact angle remained relatively high, ∼135°, and the toluene–water separation efficiency in equal parts was recorded as 100%. Fig. 5c shows images of coating E (SiO2 5–15 μm particles (0.6 g) with TiO2 21 nm particles (0.6 g) in a 0
:
1 polymer mixture of Sylgard® 184 and FAS) on copper 100 mesh substrates (149 μm pore dimensions). Open pore structures were conserved, due to the absence of Sylgard® 184, and there was a clear presence of protruding micro and nanoscale particles. The associated average water contact angle and toluene–water separation efficiency in equal parts were 147 ± 1° and 99 ± 1% respectively. Lastly, Fig. 5d displays coating F on a copper 100 mesh substrate (TiO2 60–200 nm particles (1.5 g) with TiO2 21 nm particles (1.5 g) in a 1
:
4 polymer mixture of Sylgard® 184 and FAS). The small pores were ∼50% blocked by this polymer mixture making this an unsuitable solvent–water separation device despite preserving dual scale surface contours, average water contact angle of 146 ± 1°. SEM analysis lead to the assumption that coatings with high proportions of the non-viscous fluorinated FAS polymer mixture created highly structured surface topographies and maximised the appropriate pore area of copper 60 mesh (and in some cases copper 100 mesh) substrates. This in turn elevated the average contact angle values and enhanced efficiency of solvent separation; low Sylgard® 184 levels were tolerated to preserve device coating robustness.
:
0, 0
:
1, 1
:
1, 1
:
4 and 1
:
9 Sylgard® 184
:
FAS polymer ratios with embedded hydrophobic-SiO2 (H-SiO2) and/or TiO2 loading combinations and functionally contrasted. With the majority of polymer combinations dual scale H-SiO2 particles produced the lowest average water contact angle values, for example 125 ± 10° was obtained with the 0
:
1 Sylgard® 184
:
FAS polymer ratio mixture. Dual scale TiO2 particles consistently generated the highest average water contact angle results for each coating composition (with the exception of the Sylgard® 184
:
FAS ratio of 1
:
0), a maximum of 151 ± 7° was achieved with the 1
:
9 Sylgard® 184
:
FAS polymer mixture. The coatings that contained the highest concentration of Sylgard® 184 often performed comparatively worse than mesh coatings with a larger FAS content. These findings were expected, the abundance of –C–F polymer bonds in FAS is known to effectively reduce a material's surface energy and consequently increase the average water contact angle value. All samples were in the Cassie–Baxter regime, assumed from low tilting angle results, and improved upon the hydrophobicity of separation meshes detailed in the literature. Fore example. Xue's group generated a superhydrophilic mesh whilst Zhang's coated mesh afforded average water contact angles < 130°.36,37
Average percentage of toluene separated from 25%, 50% and 75% toluene solutions (75%, 50% and 25% water respectively) were contrasted on coated 60 mesh copper substrates, via the setup in Fig. S3.† The H-SiO2 and TiO2 particle combination, B, embedded in a 1 to 9 Sylgard® 184
:
FAS mixture was the most effective at separating 25% toluene–50% water solutions on copper 60 mesh substrates (95 ± 6% separation efficiency). Fig. 7 illustrates that all H-SiO2/TiO2 particle combinations, A, B and C, reached 100% separation efficiencies for 50% toluene–50% water solutions when coupled with their optimised Sylgard® 184
:
FAS polymer mixture. Subsequently, high separation efficiencies of 99 ± 1% were achieved on dual scale H-SiO2 as well as H-SiO2/TiO2 containing particle systems embedded in a 1 to 9 Sylgard® 184
:
FAS mixture when tested with 75% toluene–25% water solutions. All particle and polymer mixture combinations had slightly reduced separation efficiencies for 25% toluene–75% water solutions but remained >90%.
Final separation efficiencies on optimised coatings on copper 60 and 100 separation meshes have been recorded in Table S2.† Coating D (SiO2 5–15 μm particles (0.6 g) with TiO2 21 nm particles (0.6 g) in a 1
:
9 polymer mixture of Sylgard® 184 and FAS) coating E (SiO2 5–15 μm particles (0.6 g) with TiO2 21 nm particles (0.6 g) in a 0
:
1 polymer mixture of Sylgard® 184 and FAS), coating F (TiO2 60–200 nm particles (1.5 g) with TiO2 21 nm particles (1.5 g) in a 1
:
4 polymer mixture of Sylgard® 184 and FAS) and coating G (SiO2 5–15 μm particles (0.6 g) with TiO2 21 nm particles (0.6 g) in a 1
:
4 polymer mixture of Sylgard® 184 and FAS) were functionally tested using various solvent systems. Table S2† documents solvent separation efficiencies for toluene–, hexane– and dichloromethane–water solutions along with associated errors.
The results indicated that coated copper 60 mesh substrates again were most likely to generate a favourable separation efficiency when compared to coated copper 100 mesh substrates. The larger pore diameter remained unblocked after coating with even the most viscous of polymer mixtures and therefore allowed toluene, hexane and dichloromethane to filter through the mesh; small pore 100 mesh substrate blockages most strongly inhibited the densest solvent, dichloromethane, from filtering through the device and consequently has not been featured in Table S2.† Despite the exceptional performance of all optimised coatings D–G, formulation F on 60 mesh substrates was an extremely effective separation coating with 100 ± 0%, 85 ± 0% and 97 ± 0% efficiencies for toluene–, hexane– and dichloromethane–water solutions respectively. The innately hydrophobic dual scale TiO2 particles embedded coating F's 1
:
4 Sylgard® 184
:
FAS mixture helped elevate the average water contact angle, 146 ± 1°. This favourable particle combination coupled with the relatively high proportion of FAS in the coating elevated average contact angles and improved separation potential. Various other separation materials that used longer more elaborate fabrication procedures have been well documented over recent years. Separation efficiencies ∼ 95% were achieved but the vast number of readily available oils/solvents and the absence of a standardized separation method makes it difficult to directly contrast like results from across the field.36–41
Due to the adhesive properties of Sylgard® 184, optimised coatings D, F and G remained comparably functional, within the original error limits represented in Fig. 6, after 3 wash–separation–wash cycles and the Scotch tape test. Fig. 8 displays the water contact angle image post separation testing of coating D; unaltered water repellency further supports coating robustness. The 1
:
9 and 1
:
4 Sylgard® 184
:
FAS ratios provided the ideal particle embedded polymer systems to preserve surface morphology and pore structures (copper 60 mesh substrates), establish preferred wettabilities and achieve surface durability.
The most favorable separation meshes were identified as a result of ensuring surface morphologies and open pore structures were preserved whilst tailoring the surface energy to reside between that of oil and water (approximately between 30 mN m−1 and 70 mN m−1).42 Trends were identified that indicated solvent density had a significant part to play. For example, copper 100 mesh separation rates were substantially higher using toluene–water solutions as opposed to hexane for identical surface coatings. This was attributed to toluene's increased density of 865 kg m−3,43 as opposed to 672 kg m−3 for hexane.44 A denser solvent was able to more quickly permeate a mesh substrate when originally mixed with water.
:
FAS polymer ratio mixtures were explored in order to enhance surface wettabilities. Average water contact angles were linked to improved solvent separation efficiencies, which, in turn, were most favourable on samples with higher quantities of the fluorine-rich fluoroalkylsilane, FAS, polymer. For example, coating F's dual scale TiO2 particle system embedded in a 1
:
4 Sylgard® 184
:
FAS polymer mixture was applied to copper 60 mesh substrates (pore diameter of 250 μm). The resulting device was highly functional with 100 ± 0%, 85 ± 0% and 97 ± 0% separation efficiencies for toluene–, hexane– and dichloromethane–water solutions respectively. A trade-off between the highly adhesive and durable Sylgard® 184 polymer and the low surface energy FAS, in a 1
:
4 ratio, afforded robust separation coatings that showed no deviation in functionality after 3 wash–separation–wash cycles nor after the Scotch tape test.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c9ra02700a |
| This journal is © The Royal Society of Chemistry 2019 |