Open Access Article
Pichkari
Saikiran
,
Mayuri
Dhole
and
Nandini
Bhandaru
*
Department of Chemical Engineering, Birla Institute of Technology and Science Pilani, Hyderabad Campus, Pin – 500 078, Telangana, India. E-mail: nandini@hyderabad.bits-pilani.ac.in
First published on 25th January 2023
Due to the increased industrial oily wastewater, developing a successful oil/water separation mechanism is a ubiquitous challenge. As oil/water separation is an interfacial phenomenon, a straightforward way is to utilize the special wettability of novel materials towards oil and water. In this work, we intend to construct a durable membrane/mesh that can have a selective response towards oil and water based on the difference in surface tension. Graphene oxide (GO) is one such material that exhibits in-air hydrophilicity and underwater superoleophobicity. GO-coated wire meshes can act as membranes with excellent efficiency for oil/water separation, but they lack long-term durability for repeated use under different environments. We created GO*-coated wire meshes by dip coating multiple layers of GO with intermediate air plasma treatment. While the multiple steps of coating ensured complete coverage of the mesh with GO, plasma treatment improved the binding of the GO coating to the wire mesh. After coating five GO layers, the mesh is subjected to mild plasma treatment to improve the porosity. The GO*-coated mesh is extremely hydrophilic in air, and the underwater oil contact angles (CA) are ≥125° for different oils. To test the long-term durability, the GO*-coated mesh is continuously immersed underwater in acidic and basic media, and the underwater oil CA is measured at different immersion times. The initial durability results are very promising and show that the GO*-coated mesh retains a significant level of underwater oleophobicity even after 60 days of continuous immersion in water.
For achieving oil/water separation, we need to target properties that are very different between oil and water. The surface tension of water is ∼72.8 mJ m−2, whereas, for most oils, surface tension is below 30 mJ m−2. Thus, by creating porous membranes/meshes that have selective responses based on the surface tension of the liquid, one can achieve effective oil/water separation. Much research has been reported in this regard with the emergence of biomimetic water-repelling (superhydrophobic) and oil repelling (superoleophobic) surfaces inspired by the surface features of lotus leaves and springtails.1,2 Novel materials with unique micro and nanoscale surface structures have been ingeniously designed to achieve both superhydrophobic and superoleophobic properties.14–16 But for the required oil/water separation, we need to fabricate materials that are either superhydrophobic/superoleophilic (high affinity towards oil) or superoleophobic/superhydrophilic (high affinity towards water).4–7 In the first approach, the oil phase will spread quickly on the surface and penetrate it (in the case of a porous membrane), while the water phase will be repelled, resulting in oil/water separation.17 However, as oil has a lower density than water, it is challenging to design an efficient separation technique for large-scale applications. Moreover, oil-removing membranes easily become fouled and clogged by the oil due to the oleophilic properties, reducing the separation efficiency.4 The second approach of superoleophobic/superhydrophilic surfaces/membranes also has several limitations. Oil has a much lower surface tension than water, due to which a superhydrophilic surface exhibits superoleophilicity. In addition, making any surface oleophobic is not easy as there are no chemicals available that can directly achieve this property. Superoleophobicity has only been achieved by making specific micro and nanoscale structures with fluorinated polymers, which can be a complicated multi-step process.4 However, the study of fish scales a decade ago showed that they are highly hydrophilic and, therefore, can exhibit superoleophobicity underwater and protect the fish from contagion by oil pollution in the sea.18 This inspired the most effective and straightforward oil/water separation techniques reported till now based on membranes/meshes showing superhydrophilicity at the air/solid interface and superoleophobicity at the water/solid interface.
One of the first works on oil/water separation using a superhydrophilic and underwater superoleophobic mesh was reported by Xue et al. using PAM hydrogel-coated stainless steel meshes to separate water from oil/water mixtures with >99% efficiency.19 However, hydrogels can swell quickly in water and have weak stability. Several other techniques and materials have been used since then for better functionalization of meshes. Coatings of organic materials such as polymers, block copolymers, polyelectrolytes, polymer blends, and polymer brushes have been extensively used to create hydrophilic water-selective meshes.7,20–23 Copper (Cu), copper oxide, or copper hydroxide-based nanostructure-coated meshes have been the most widely reported inorganic functionalization techniques to obtain water-selective meshes.3,24,25 Zhang et al. reported Cu(OH)2 nanowire-haired copper mesh that can effectively separate oil/water mixtures and oil-in-water emulsions and provide long-term anti-fouling properties.24 Apart from Cu, silica particles, carbon nanotubes, titanium dioxide nanoparticles, zeolites, and several other materials have also been used to functionalize metal meshes better. All the reported meshes with organic or inorganic materials have reasonable oil/water separation efficiency, but they either fail to give high filtrate flux or have poor chemical stability.5,6 For better stability, direct etching of the metallic meshes using the laser ablation technique has been used for making more reusable meshes. But the method can be costly for large-scale oil/water separation. Recently, Lian et al. reported a nanosecond laser ablation technique to modify brass mesh, which they claim is low cost and more economical compared to previous methods.26
Of all the reported materials, graphene oxide (GO) coated membranes can be considered unique because of the layered nanostructure resembling that of fish scales or clamshells, abundant oxygen-containing functional groups, and excellent hydrophilicity, making them promising 2D meshes for oil/water separation.27–31 Recently, simple GO coatings on brass or steel wire meshes have been reported with high separation efficiency. Dong et al. reported for the first time in 2014 that GO-coated stainless steel meshes have extraordinary hydrophilic and underwater superoleophobic properties and can be used for gravity-driven oil/water separation.27 The GO-coated meshes showed very low oil-adhesion characteristics and separation efficiency above 90% with all types of oils. Liu et al. used O2 plasma treatment after coating GO on the stainless-steel mesh to open clogged pores and change the pore diameter.28 They achieved high separation efficiency even after 50 cycles of oil/water separation. Both works mention that finer meshes (300 or 400 mesh) with pore diameter of ∼40 μm were best suited for oil/water separation. While GO coated meshes have been proven to be highly effective and promising for large-scale oil/water separation applications, to achieve a reasonable flux rate at low cost, we need to depend on a coarser mesh with larger pore size, and for long-term usage of these meshes, we need to have the excellent chemical stability of the GO coating.31 Notably, for marine applications, the long-term effect of continuous immersion underwater on superoleophobicity must be checked.32
In this work, we report the preparation of a stable underwater superoleophobic mesh by dip-coating GO on a brass mesh. Air plasma treatment of the mesh was done before and after the GO coating steps. The initial plasma treatment of the bare mesh helped improve the adhesion between the GO and the metallic mesh. The dip-coating of GO was done multiple times to achieve complete coverage and a layered texture. After dip coating, the second plasma treatment resulted in the etching and opening of the fully obturate mesh pores. We also checked for the long-term durability of the GO coating on the wire mesh for the first time upon continuous immersion of the mesh in acidic, basic, and neutral media, mimicking the usual properties of industrial oily wastewater. We observed that the plasma-treated meshes remained superoleophobic underwater even after 60 days of immersion, while the untreated samples showed leaching of the GO coating within a couple of hours. We show that the plasma treatment steps significantly enhance the long-term stability and chemical durability of the GO coating on the wire mesh.
:
1) were stirred, and 3.0 g of graphite flakes was added as depicted in step 1 of Fig. 1. In step 2, 18.0 g of potassium permanganate (KMnO4, SRL) was slowly added under continuous stirring conditions. Stirring was done continuously for at least 20 hours, maintaining the temperature at 40 °C until the solution became dark green. The reaction mixture was then cooled to room temperature and then poured onto a mixture of 400 g of ice and 3 mL hydrogen peroxide (H2O2, Avra). During this step, ice was added to decrease its viscosity and avoid overheating, while H2O2 helps in the easy removal of metal salts like permanganate and manganese residuals from the mixture. Then, the mixture was centrifuged at 5000 rpm for 2 h (step 3, Fig. 1). After the decantation of the supernatant, the solid residuals were washed with 200 mL of hydrochloric acid (35% HCl, SD) and 200 mL of DI water in succession 3 times. Finally, the solids obtained after multiple rounds of washing were dried in an oven at 90 °C for 24 h to give 3.25 g of GO powder.
O and C
C bonds, respectively, which confirms the presence of the carboxylic acid group and aromatic groups. The band at 1395.24 cm−1 can be due to the stretching of the C–OH group in water molecules soaked onto GO sheets. Similarly, the bands at 1219.75 cm−1 and 1044.56 cm−1 can be due to the stretching of C–O (epoxy) groups. Fig. 2B shows the XPS C 1s spectra of the as-prepared GO powder. After deconvolution, it is distinctly apparent that the C 1s spectrum contains four peaks at 284.78 eV, 286.88 eV, 288.68 eV, and 289.78 eV, which are attributed to the C
C bond (in the aromatic ring), C–O bond (in hydroxyl and epoxy groups), C
O bond (carbonyl group) and O–C
O (carboxyl group) respectively. We can clearly infer from the intensities of the peaks that GO has been oxidized satisfactorily.33Fig. 2C and D show the AFM and FESEM images, respectively of the GO sheets on the silicon wafer substrate. Both AFM and FESEM images show the presence of thin sheets along with wrinkle-like structures on the GO surface. This wrinkle formation may have been observed due to the coating and the drying process on the substrate.36 To check the level of oxidation and hydrophilicity, the GO powder was dispersed in water and mixed with an equal amount of different non-polar solvents with vigorous shaking by hand. The nonpolar solvents used were kerosene, toluene, petroleum ether, hexane, chloroform, and edible sunflower oil, as shown in Fig. 2E. As the dispersion settled, we observed that most of the GO was present in the water phase proving the hydrophilic properties of GO. Some amount of GO was also seen in the interface between water and the non-polar solvents, as GO can also act as an amphiphilic material due to the sp2 conjugated system.27
Fig. 3A shows the OM images of the brass mesh (∼300 μm pore size) after cleaning and plasma treatment. The initial plasma treatment was done to remove any impurities, increase the surface energy and oxidize the surface for better binding of GO to the mesh. To achieve uniform coverage of GO on the mesh, we dip-coated the mesh with the GO dispersion five times with intermediate drying after each coating. Fig. 3B shows the mesh after applying three coats of GO. After coating five times, we observed that most of the pores in the mesh were covered with a continuous GO film, as seen in Fig. 3C. To open the fully obturate pores, the mesh was subjected to air plasma treatment from one side for 1 min.28 Plasma treatment leads to strong oxidation and etching of GO from the pores of the mesh while the GO coating on the opposite side of the mesh remains intact. After treatment, we obtained a GO*-coated mesh with all open pores with an average pore size of 202 ± 15 μm, as seen in Fig. 3D. While applying multiple layers of coating helps in ensuring uniform coverage of the mesh with GO, the final plasma treatment can be used to open pores with control of pore size.
The in-air wettability and underwater oleophobicity of the mesh were quantified using contact angle (CA) measurements. The bare mesh showed slight hydrophobicity in the air with a CA of ∼92.7° ± 1.6°. The image of a water drop on the brass mesh is shown in Fig. 4A. The GO-coated mesh was hydrophilic with an initial CA of 81.3° ± 2.2° which reduced to 29.0° slowly over 15 min as water permeated through the mesh (Fig. 4B). Upon coating GO following our protocol which includes plasma treatment steps, we observed an initial CA of 74.3° ± 2°. The water drops quickly permeated through the GO*-coated mesh, and the CA reduced to 5.5° within 30 s, and the drop fully disappeared (Fig. 4C). The improved hydrophilic nature of the GO*-coated mesh and open pores obtained after plasma treatment makes water permeate through the membrane very quickly, which is an essential property for high flux underwater oil/water separation application. The underwater oil CA was measured by placing the mesh samples upside down and immersing in water near the top of a water bath. Drops of oil or organic solvent like toluene were created in the water bath and were allowed to deposit on the mesh as the drops moved upwards due to density difference. The CA data and images of oil drops on bare mesh, GO-coated mesh, and GO*-coated mesh are shown in Fig. 4D for edible oil, toluene, and kerosene. The GO*-coated mesh showed a CA of 130° or above for the three oils, whereas the GO-coated mesh showed a CA of above 110° for the three oils. The bare mesh showed CA between 85° and 105°. This is a considerable improvement in oleophobic properties for a coarse mesh with ∼300 μm pore size. The reason behind the underwater oleophobicity of the GO*-coated mesh is its super hydrophilicity which is a combined effect of GO coating and plasma treatment. Typically, the liquid CA and wettability on a solid surface in the air are determined using Young's equation.1 Young's equation can be modified for different settings, including the determination of CA of a liquid on a solid surface immersed in a second liquid.18 The modified equation can be written as:
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The durability of the coating on the mesh is a significant factor in determining the long-term usage of the mesh in applications such as oil/water separation. While a myriad of fabrication techniques have been proposed to date, the foremost challenge with all the techniques is the poor durability against external influences.4 Many works have reported the stable separation efficiency of the membranes after repeated cycles of oil/water separation tests. Some of the works went one step ahead and tested chemical and thermal stability by using water/oil mixtures containing hot water, acidic water, basic water, or salt.28,31,37 But only a few groups have studied the long-term durability and chemical stability of the meshes when immersed in a medium for durations up to 24 h.37 To better understand the long-term durability of the GO*-coated mesh and the stability of the superoleophobic properties of the mesh, we immersed the GO*-coated mesh samples in water, acidic medium, and basic medium continuously for up to 60 days. We took out different samples at intermediate durations, dried them naturally, and imaged and measured the underwater oil CA.
Fig. 5A and B show the GO-coated mesh and GO*-coated mesh immersed in water, respectively. Upon continuous immersion for 10 days, we observed that the GO-coated mesh started leaching out, and the GO flakes dispersed into the water slowly, as seen in Fig. 5A. Under an OM, we can see that the coating is missing from several parts of the mesh, as shown in Fig. 5E. For the GO*-coated mesh samples, we did not see any GO flakes leaching out even after 60 days of continuous immersion (Fig. 5B). This experiment gives preliminary proof that the initial step of plasma treatment has helped in improving the adhesion between GO flakes and the brass mesh. Fig. 5F shows the OM image of the mesh after 60 days of continuous immersion in water. We can see that the mesh is still coated with the GO and looks similar to the GO*-coated mesh shown in Fig. 3D.
In a low pH medium, it has been reported that the carboxyl groups of the GO sheets become protonated, lose their hydrophilic properties, and form aggregates.38 When GO*-coated meshes were immersed in an acidic medium, we observed a similar process of gradual formation of aggregates in the medium, which was clearly visible after 60 days of continuous immersion, as seen in Fig. 5C. The formed aggregates may detach from the mesh and remain suspended in the medium. Fig. 5G shows the OM image of the same mesh in which the GO coating around the wire mesh appears to be swollen with pore size ∼ 63 ± 2 μm. The swelling can be due to the protonated carboxyl groups of GO in an acidic medium, which can form stable layered aggregates of GO and water.38,39 In a basic medium, the ionization of the carboxylic groups may cause the dissolution of GO sheets into the medium.39 While we did not observe any change in the color of the basic medium even after 60 days of continuous immersion, the brass mesh became very brittle and corroded due to dezincification in the high pH medium (Fig. 5D). The dissolution of the GO coating exposed the brass mesh which caused faster corrosion. Fig. 5H shows that the pore size of the mesh in the basic medium has been reduced to ∼50 ± 8 μm, and a few pores have closed up.
For the GO-coated mesh, after ten days of continuous immersion in water, the underwater edible oil CA reduced from 138.2° to 90.0° (35% reduction). The leaching of GO flakes reduces the oleophobicity, and the edible oil CA was similar to that of the bare mesh. In contrast, for the GO*-coated mesh, the edible oil CA reduced from 141.0° ± 3.0° to 135.0° ± 0.6° (4% reduction) after ten days of continuous immersion in water. Fig. 5I shows the variation in the underwater edible oil CA when the GO*-coated mesh is immersed continuously in water, acidic medium and basic medium for different durations of time up to 60 days. In the neutral medium, the GO*-coated mesh remains significantly oleophobic with an underwater edible oil CA of 112.0° ± 3.0° after 60 days of immersion (20.6% reduction). This shows that the GO*-coated mesh is much more durable than the GO-coated mesh. In an acidic medium, the formation of aggregates and leaching of GO flakes affected the oleophobicity as the edible oil CA dropped to 99° ± 1.0° after 60 days (30% reduction). The basic medium caused maximum degradation of the GO coating as the edible oil CA dropped to 54° ± 8.0° (61.7% reduction). Still, Fig. 5I confirms that all the GO*-coated meshes maintain significant oleophobicity (underwater oil CA > 120°) after 20 days of continuous immersion.
Apart from oil CA, another important physical property for oil/water separation application is the breakthrough pressure, the maximum pressure required to make the liquid permeate through the mesh.6 For an underwater superoleophobic mesh, the breakthrough pressure, ΔPwC, depends on rP (radius of the mesh pores) and is given as:
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For the GO*-coated mesh, the theoretical value of ΔPwC was calculated to be 621.7 Pa, for rP = 101 μm. Upon continuous immersion in water, acidic medium and basic medium for 60 days, the theoretical ΔPwC reduced to 272.4 Pa, 198.6 Pa and −940.5 Pa respectively. This shows that along with degradation of superoleophobicity, the maximum pressure that the mesh can withstand also reduces. A negative value of ΔPwC in the basic medium indicates that the oil will spontaneously penetrate through the mesh without any external force and the mesh cannot be used for oil/water separation. Using ΔPwC = hmaxρg (ρ is the density of edible oil, g is the acceleration due to gravity, and hmax is the maximum height of the edible oil column that the mesh can support), the theoretical value of hmax over a fresh GO*-coated mesh was ∼6.9 cm. We also measured the stability of a 10 cm oil column over the GO*-coated mesh and found that the oil column remains stable over the mesh even after 30 min of observation. This shows that the experimental value of the breakthrough pressure for the mesh was ∼900.4 Pa.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2na00667g |
| This journal is © The Royal Society of Chemistry 2023 |