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Review

Recent Advances in Femtosecond Laser-Induced Surface Structuring for Oil–Water Separation

by
Ali Sami Alnaser
1,2,*,
Sharjeel Ahmed Khan
1,2,*,
Rashid Ashirovich Ganeev
2 and
Emmanuel Stratakis
3,4
1
Department of Physics, American University of Sharjah, Sharjah 26666, UAE
2
Material Science and Engineering Research Institute (MSERI), American University of Sharjah, Sharjah 26666, UAE
3
Institute of Electronic Structure and Laser, Foundation for Research and Technology-Hellas, 71110 Heraklion Crete, Greece
4
Department of Physics, University of Crete, 71003 Heraklion Crete, Greece
*
Authors to whom correspondence should be addressed.
Appl. Sci. 2019, 9(8), 1554; https://doi.org/10.3390/app9081554
Submission received: 19 March 2019 / Revised: 3 April 2019 / Accepted: 10 April 2019 / Published: 15 April 2019
(This article belongs to the Special Issue Ultrafast Laser Pulses)
Browse Figures
Versions Notes

Abstract

:
Femtosecond (FS) laser-induced surface structuring is a robust, maskless, non-contact, and single-step process for producing micro- and nanoscale structures on a material’s surface, which remarkably alters the optical, chemical, wetting, and tribological properties of that material. Wettability control, in particular, is of high significance in various applications, including self-cleaning, anti-fouling, anti-icing, anti-corrosion, and, recently, oil–water separation. Due to growing energy demands and rapid industrialization, oil spill accidents and organic industrial discharges frequently take place. This poses an imminent threat to the environment and has adverse effects on the economy and the ecosystem. Oil–water separation and oil waste management require mechanically robust, durable, low-cost, and highly efficient oil–water manipulation systems. To address this challenge superhydrophobic–superoleophilic and superhydrophilic–underwater superoleophobic membrane filters have shown promising results. However, the recyclability and durability issues of such filters are limiting factors in their industrial application, as well as in their use in oil spill accidents. In this article, we review and discuss the recent progress in the application of FS laser surface structuring in producing durable and robust oil–water separation membrane filters. The wide variety of surface structures produced by FS laser nano- and micromachining are initially presented here, while the excellent wetting characteristics shown by specific femtosecond-induced structures are demonstrated. Subsequently, the working principles of oil–water separation membranes are elaborated, and the most recent advances in the topic are analyzed and discussed.

1. Introduction

Surface structuring using femtosecond (FS) pulses gives rise to spatially resolved micro/nanometer-sized features that are attributed to the reduced thermal and mechanical effects upon the ultrafast laser–material interaction [1,2]. It is a novel technique for precise control of a wide range of properties on virtually any type of material, including optical, mechanical, chemical, wetting, biological, and tribological properties [3]. As a result, FS laser-induced surface structures are used in a broad range of applications, including plasmonics, photonics, optoelectronics, photovoltaics, biomedicine, microfluidics, self-cleaning, and oil–water separation. For example, highly absorptive, black metallic [4], and semiconducting [5] surfaces formed by FS laser structuring are used in photovoltaics [6], as well as in stealth technology [7], to entirely absorb ultraviolent -visible (UV–Vis) and infrared (IR) radiation. In addition, FS laser-fabricated, pigment-free, colored metals [8,9] and iridescent surfaces [10] can be applied for the fine-tuning of surface optical properties. Such colors are due to the plasmonic absorption at specific wavelengths featured by the laser-induced surface structures. Moreover, FS laser surface structuring can significantly alter the wetting properties of different materials. Inspired by the lotus leaf found in nature, superhydrophobic surfaces have been generated for applications in self-cleaning, anti-icing, drag reduction, corrosion resistance, and water harvesting [11,12,13]. In contrast to superhydrophobic surfaces, FS laser structuring can also provide, under certain irradiation conditions, surfaces capable of engulfing significant amounts of liquid, called super-wicking surfaces [14,15]. This effect is so strong that liquid could be transported uphill, against the gravitational pull, onto the structured surface. Recently, wettability control by varying the number of pulses and laser fluence in titanium [16] and copper [17], respectively, has been achieved by FS laser processing. It has been found that the number of incident pulses, pulse energy, laser fluence, and environment are important factors in realizing different levels of wettability [18,19]. Moreover, superhygrophobic surfaces recently fabricated by FS laser are able to repel complex liquid droplets, such as glucose, cola, juice, saline, and bovine serum albumin in water [20]. Other applications of FS laser-induced surface processing include the structuring of tissue engineering scaffolds showing enhanced cell adhesion properties [21,22,23], signal intensification for surface-enhanced Raman spectroscopy [24], enhancement of X-ray generation and photoelectron emission and manipulation of tribological properties [25,26].
The superior precision and accuracy of FS laser-induced surface structuring is a direct consequence of the shorter pulse duration and, thus, the laser–material interaction time [27]. In the case of longer pulses, the thermal energy generated upon melting diffuses around the irradiation spot, giving rise to the creation of heat-affected zones (HAZs). Above the material damage threshold, the HAZ has a detrimental effect on the integrity of the material by producing microcracks together with micropores. Besides this, when using longer pulses, the ablated material causes recast layers and surface debris, resulting in poor fabrication resolution. All such effects are avoided upon using FS laser pulses, due to the faster ablation process, i.e., rapid vaporization and material removal. Furthermore, FS laser surface structuring has various advantages compared with other techniques, such as photolithography, electron or ion beam; andmechanical and chemical methods. Such techniques involve multiple steps and tedious sample preparation and require vacuum conditions and hazardous chemicals. In conclusion, FS laser surface structuring is a simple, maskless, single-step, and non-contact process, enabling the controllable fabrication of various complex two-dimensional (2D) and three-dimensional (3D) structures [28,29,30,31,32,33] with high precision, as presented in Figure 1.
The interaction of FS laser pulses with matter involves several processes and phenomena, taking place on short timescales. During the first moments of interaction, instantaneous excitation of electrons occurs due to linear or non-linear photon absorption processes. The former takes place in metallic materials—contrary to semiconducting and dielectric ones—where non-linear absorption processes become more pronounced. As a result of photon absorption, the electron temperature increases to much higher values compared with that of the lattice, because electron–electron interaction is much faster than electron–phonon coupling. Subsequently, the hot electrons and cold lattice reach equilibrium in a few picoseconds through electron diffusion and electron–phonon interaction [34]. This two-temperature model is widely used to interpret the laser–matter dynamics on the electronic level, prior to the establishment of thermal equilibrium. With regard to laser-induced surface structures, the electron–phonon interaction is a key factor in understanding their formation. In particular, the energy transfer from the electrons to the lattice depends on the electron–phonon coupling constant; the higher this constant, e.g., in metals, the faster the electron-to-lattice energy transfer occurs [34]. Furthermore, the energy accumulation on the material’s surface and, therefore, the hydrodynamics of the molten pool leading to laser-induced self-assembled structures under non-ablation conditions [35] are highly dependent on the electron–phonon coupling constant.
Figure 2 shows the typical setup for FS laser-based surface structuring. The laser beam from the FS laser source is focused on the sample mounted on an XYZ translation stage controlled by a computer program. A combination of proper optics and lenses guides the laser beam to the sample. An electromechanical shutter placed in the beam’s path interrupts the laser beam in raster scanning or spot-by-spot processing after a particular number of laser shots. The joulemeter is used to measure the energy deposited on the surface of the sample in real time. By controlling the laser fluence, wavelength, repetition rate, number of pulses, and pulse duration, various surface structures are formed on different materials.
Over the last decade, FS laser-induced surface structures have been successfully used to control the wetting response of materials [12], especially for the fabrication of surfaces exhibiting extreme wetting properties, from superhydrophobic to superhydrophilic and from superoleophobic to superoleophilic. Due to their remarkable superwetting characteristics, FS laser surface structures have recently been employed for applications in oil–water separation. In this article, we will critically review the extreme wetting properties reported for the FS laser-induced surface structures, as well as the research progress on the production of oil–water separation membranes by means of FS laser micro/nano fabrication.

2. Femtosecond Laser-Induced Self-Organized Periodic Surface Structures (LIPSS)

Apart from the complex, patterned surfaces attained by FS laser micromachining under ablation conditions, surface processing by FS lasers can also give rise to various submicron- and micron-sized, self-organized laser-induced periodic surface structures (LIPSS) created under practically non-ablative conditions [27,35]. Figure 3 represents an example of the different LIPSS structures attained on silicon upon irradiation with different numbers of FS pulses at a constant incident fluence. With a low number of pulses, the formation of laser-induced surface ripples perpendicular to the laser beam polarization occurs. Upon increasing the number of pulses, the formation of supra-wavelength laser-induced surface grooves (LISG), oriented parallel to the beam polarization, takes place. Further increasing the number of incident pulses gives rise to the creation of a quasi-periodic array of FS laser-induced surface micro-spikes (LISS) [2].

2.1. Laser-Induced Surface Ripples

Laser-induced surface ripples (LISR) are formed on solid surfaces when the polarized laser beam interacts with a material, generating a periodic spatial distribution of the electromagnetic field and, in turn, a periodic spatial distribution of the melt profile at micrometer and sub-micrometer scales. LISR are widely studied, and a broad variety of such structures can be created due to their dependence on laser fluence, number of pulses, angle of laser beam incidence, wavelength, and polarization direction. The LISR formation mechanism and its dependence on various parameters have already been reviewed in [36]. Although LISR have been generated by long laser pulses [37], the advancement of FS lasers has revealed exciting ways to create such structures with improved spatial resolution. LISR have found applications in creating different structural colors [9,38] and anti-reflecting coatings [4,7] and in controlling surface wetting properties [39].
Given that the LISR formation and orientation are directly related to the laser polarization state [40,41], control over the beam polarization is a unique tool to fabricate complex LISR morphologies comprising more than a single spatial frequency, as shown by LISR fabricated with linearly polarized light [30,40]. Such frequencies can be efficiently tuned upon variation of the central laser wavelength and the number of pulses per irradiation area [36]. Figure 4 presents examples of complex LISR structures fabricated upon laser processing with three different polarization states on Ni [30] surfaces. Considering that wetting properties are highly dependent on the shape, size, and orientation of the surface structures, the polarization control of LISR should be a useful tool to realize an ensemble of complex morphologies, facilitating the elegant tuning of the wettability of materials used for oil–water separation.

2.2. Microgrooves

Although LISR formation occurs for low excited electron densities, laser-induced surface grooves (LISG) appear for large ones. The increased temperature due to the relaxation process leads to a thermal gradient and the formation of convection rolls in the molten material because of the Marangoni effect, which eventually leads to sub-wavelength microgrooves [35]. As confirmed by both experimental studies and simulations, the LISG periodicity is an increasing function of the number of pulses [35]. LISG show higher superhydrophobicity compared with LISR and, therefore, are expected to be good candidates for oil–water separation [42].

2.3. Conical Spikes or Columnar Structures

Conical or columnar structures can also be formed by laser surface structuring at optimized fluence, ablation threshold, number of pulses, scanning speed, and type of material [43]. For example, Figure 5a–d shows columnar structures covered with nanostructures on a titanium surface with a TiSa Laser (65 FS, λ = 800 nm, 1 kHz, 0.35 J/cm2) at different numbers of pulses. It was observed that columnar structures began to form when the laser exposure reached 100 shots, while they became more prominent upon increasing the number of pulses [21]. This finding indicates that the geometrical features of columnar structures can be manipulated by optimizing the number of incident pulses. Moreover, the pulse energy and the type of material are additional factors that need to be considered. Indeed, the higher damage threshold for hard materials (e.g., for titanium it should be above 0.5 J/cm2 [44]) and the lower one for soft materials (e.g., for aluminum it should be below 0.16 J/cm2 [44]) need to be taken into account upon optimizing the columnar structures. Furthermore, the irradiation environment may influence the formation of conical structures. For instance, conical structures grown on titanium [45] and silicon [2] are taller and sharper when irradiated in the presence of SF6 gas. Figure 5e,f shows an Si surface irradiated in air and a SF6 gas environment with an average of 500 laser pulses (180 FS, λ = 800 nm, F = 2.47 J/cm2). The conical structures show remarkable superhydrophobicity compared with LISR and LISG [42]. Therefore, such structures are expected to be promising candidates for oil–water separation.

3. Wettability Control

The wetting properties of materials have great significance in a wide range of applications and are thus critical for understanding the mechanism of oil–water separation. The wettability of a material comes as the result of the synergy of the surface morphology and chemistry [46]. Inspired by the remarkable superhydrophobic properties of the natural lotus leaf, researchers have mimicked the leaf morphology and surface chemistry to produce artificial surfaces showing extreme water repellency [47]; water droplets do not wet and bounce as a perfect elastic sphere on such surfaces and easily roll off, giving rise to a self-cleaning effect. Lotus leaf microscopic analysis has revealed the presence of hierarchical surface structures, comprising microconical asperities decorated with a layer of waxy nanohairs. Such hierarchical microstructures are behind the self-cleaning features of the lotus leaf, which keep it lush, green, and clean [47]. As a consequence of such remarkable properties, artificially prepared superhydrophobic surfaces have found a wide range of applications in self-cleaning, anti-icing, anti-corrosion, drag reduction, and oil–water separation uses [48,49]. Superhydrophobic surfaces exhibit a water contact angle (WCA) higher than 150° and a roll-off angle (sliding angle (SA) in Figure 6b) lower than 10°. Based on the same principles, superoleophobic surfaces exhibit an oil contact angle (OCA) higher than 150° and a roll-off angle lower than 10°. On the other hand, superhydrophilic and superoleophilic surfaces show contact angles of ~0° for water and oil, respectively.

4. Oil–Water Separation Mechanism

The superwetting characteristic of water and oil phases on a solid surface is predominantly responsible for oil–water separation in membrane technology. The wetting response of a surface to a liquid is characterized by the contact angle of a liquid droplet on the surface. When such a droplet is placed on a surface, it forms a hemispherical shape due to the minimization of the surface free energy. The contact angle, θ, depending on the surface free energy of the solid, liquid, and vapor interfaces, is described by Young’s equation [50]:
cosθ = (γSV − γSL)/γLV
where γSV, γSL, and γLV are the surface free energy of the solid/vapor, solid/liquid, and liquid/vapor interfaces, respectively (Figure 6a).
Young’s state explains the wettability response of the material on an ideally flat surface. However, microscopic surface roughness has a crucial influence on the wetting response. The effect of the surface roughness on the wettability has been widely described by two different models (Figure 6c,d). In the Wenzel model, the liquid is assumed to completely penetrate the entire rough surface, described as a homogeneous wetting state, without leaving any air pockets underneath. The apparent contact angle, θw, is then given by a modified Young’s equation:
cosθw = r(γSV − γSL)/γLV = r cosθ
where the roughness factor “r” is the ratio of the unfolded to the projected surface area [51] and θ is the contact angle on a flat surface of the same nature as the rough. Because r is always greater than unity, this model predicts that the contact angle will decrease/increase with surface roughness for an initially hydrophilic (θ < 90°)/hydrophobic (θ > 90°) surface. In other words, a hydrophobic rough surface becomes more hydrophobic, while a hydrophilic one becomes more hydrophilic. Furthermore, contrary to the Wenzel’s droplet state, Young’s state, i.e., an ideally flat surface, exhibits limited hydrophobicity, as the effect of the surface energy alone is not enough to realize superhydrophobicity.
Contrary to the Wenzel state, in the case of the Cassie–Baxter droplet state (Figure 6d), the droplet sits on the surface microstructures, and air pockets are trapped beneath the liquid [52]. In this case, the apparent contact angle θCB is provided by the following relation:
cosθCB = f cosθ + f − 1
where f is the area fraction of the liquid in direct contact with the surface structures and θ is the Young’s contact angle. As f is always lower than unity, this model always predicts the enhancement of hydrophobicity independently of the value of the initial contact angle θ. In practice, a transitional stage between the Wenzel and Cassie state is more likely to occur, in which the liquid only partially permeates the rough surface (Figure 6e). As a result, the droplet forms a composite solid–liquid/air–liquid interface with the surface in contact. In this case, the apparent contact angle, θtr, is an average of the flat surface, θ, and the value for suspending over the flat surface (that is, 180°) is given by [53]:
cosθtr = rf f′cosθ + f′ − 1
where f′ defines the fraction of the projected solid surface that is wetted by the liquid and rf is the roughness ratio of the wet area. When f′ = 1 and rf = r, Equation (4) turns into the Wenzel equation. In the extreme case of a superhydrophilic–underwater superoleophobic surface (Figure 6f), the droplet volume is adsorbed by the surface structures in air, but when an oil droplet is placed on the surface while it is immersed in water, it exhibits a high contact angle for oil. This is explained by extending the Cassie–Baxter or transition states for the oil droplet. To realize oil–water separation, two different approaches are commonly used, namely superhydrophobic–superoleophilic membranes or superhydrophilic–underwater superoleophobic membranes. In superhydrophobic–superoleophilic membranes, oil is adsorbed while the water is obstructed due to the non-wetting properties. However, a superhydrophilic–underwater superoleophobic membrane repels oil under water. The wetting response of the latter surface depends on the medium; thus, it is superhydrophilic and oleophilic in air, but when it is immersed in water, it becomes superoleophobic. As a consequence of this response, water passes through the membrane, whereas oil is obstructed, resulting in oil–water separation.

5. Oil–Water Separation via FS Laser Structuring

Oil–water separation was realized for the first time via a superhydrophobic and superoleophilic mesh. In particular, a rough microstructured polytetrafluoroethylene (PTFE) coating deposited on stainless mesh was used for separation [54]. It was reported that when an oil–water mixture is poured on the mesh, oil gets absorbed, while water is repelled due to the superhydrophobic–superoleophilic behavior of the prepared mesh. Over the past decade, superhydophobic–superoleophilic and superhydrophilic–underwater superoleophobic membranes have been produced using different techniques on various materials. Such techniques include electrochemical deposition, sol–gel process, chemical etching, lithography, spray and dip coating; and they have been employed to modify materials such as filter paper [55], cotton [56,57], fabric [58], wood [59], metallic meshes [60], and sponges/foams [55,61] for oil–water separation [62,63]. Moreover, oil–water separation has been reported for superhydrophilic–underwater superoleophobic surfaces [64]. Although such techniques have provided promising separation efficiencies, it was impossible to retain their special wetting characteristics for a prolonged time. This can be attributed to the corrosive action of the liquids, high temperature, friction, and mechanical wear and tear [65]. Moreover, most of the produced coatings were fragile and easily worn off by slight mechanical abrasion; as a result, the super-wetting properties significantly degraded over time.
On the contrary, FS laser microfabrication has shown exceptional results with respect to the realization of durable and reliable superwetting materials for efficient oil–water separation [62]. Table 1 summarizes the most important recent reports on this topic. In particular, oil–water separation filters have been formed by either FS laser drilling of micro-through holes in a thin sheet or growing hierarchical microstructures on a mesh surface via FS laser ablation. Oil–water separation has been realized with or without subsequent chemical functionalization [11,69,71]. Recently, FS laser surface structuring has been used to produce six different types of wettability for polydimethylsiloxane (PDMS) and aluminum surfaces [72,73]. FS laser-irradiated aluminum surfaces exhibit superhydrophilic, underwater superoloephobic, and underwater superaerophilic wettability characteristics. When the FS laser-structured aluminum surface is functionalized with 1H,1H,2H,2H-perfluorodecyltriethoxysilane, its wettability behavior changes completely to superhydrophobic, underwater superoleophilic, and underwater superaerophilic [72]. In the case of a FS laser-structured PDMS surface, superhydrophobic, underwater superoleophilic, and underwater superaerophilic wetting properties were observed. Further irradiation with oxygen plasma activated the PDMS surface by inducing Si-OH groups. As a result of oxygen plasma treatment, the PDMS wettability was switched from hydrophobic to hydrophilic. Therefore, superhydrophilic, underwater superoleophobic, and underwater superaerophobic wettability were realized [73]. In light of the above results, it can be concluded that wettability control via FS laser structuring is a promising tool for oil–water separation.

5.1. FS Laser-Structured Meshes

Liu et al. reported on a Janus wire mesh for oil–water separation (Figure 7) that exhibited different wettability on its opposite sides [66]. One side was superhydrophobic–superoleophilic, while the other side was superhydrophilic–underwater superoleophobic. Initially, LISR were formed on both sides of the copper mesh, and then, the superhydrophobic side was prepared by surface functionalization with 1H,1H,2H,2H-perfluorodecyltriethoxysilane. Similarly, the underwater superoleophobic side was formed via dipping into a graphene oxide aqueous solution. Figure 7a–h shows SEM images and the elemental map of both sides of the mesh, which confirm the modification with fluorosilane and graphene oxide, respectively. It was observed that the opposite wetting responses present on the same mesh facilitate the separation of light and heavy oils from water. For light oil separation, the superhydrophobic–superoleophilic side was brought in contact with the oil–water mixture, whereas for heavy oil separation, the oil–water mixture was placed on the superhydrophilic–underwater superoleophobic side. As a result, for both heavy and light oil–water mixtures, a separation efficiency greater than 99% was achieved.
Yin et al. used a FS laser to generate LISR on stainless-steel mesh for oil–water separation purposes [67]. Figure 8a,b shows an optical image of the mesh before and after laser treatment, respectively; following the laser treatment, the mesh color turned to black. Figure 8c–e shows that the uniform nanoripples, exhibiting a 500–800 nm period and an average depth of 130 nm, are covered with nanoparticles of variable sizes, formed upon FS laser treatment. Figure 8f,g presents the chemical composition of the pristine and laser-treated meshes. The latter showed an increase in oxygen content, attributed to the oxidation of Cr, Mn, and Fe present in the stainless steel. As a consequence of the laser treatment, the mesh wettability changed from having weak hydrophobicity in its pristine state to being superhydrophilic. Moreover, the underwater contact angle of a 1,2-dichloroethane oil droplet on the laser-processed mesh was equal to 157.2°, and the sliding angle was 5°. An oil–water separation process using laser-structured mesh is demonstrated in Figure 9a–d. An oil–water mixture was poured onto the pre-wetted laser-treated mesh positioned above two beakers at a ~25° tilt angle. It was observed that water passed through the mesh and dripped off into the first beaker, while oil was repelled and rolled off the mesh surface and was collected in a separate container. Laser-treated stainless-steel mesh was tested with different oil–water mixtures, and all showed high OCAs >150°, irrespective of oil type, and a high separation efficiency of 99%. The laser-processed mesh was quite durable and chemically inert, considering that it retained its wetting characteristics even when it was rubbed repeatedly with sand paper and after being treated with 1 M HCl, 1 M NaOH, and 10% NaCl solutions. Such severe treatments validate the use of laser-structured mesh in harsh environments.

5.2. FS Laser Fabrication of Arrays of Micro-Through Holes

FS laser microfabrication was used to create rough microstructures on the surface of PTFE sheets, as shown in Figure 10a–c [68]. Following the laser ablation process, the PTFE sheet surface showed a porous structure, comprising highly dense protrusions with heights ranging from 300 nm to 2 µm. As a consequence, the laser-structured sheets showed both superhydrophobicity and superoleophilicity with static water and oil contact angles of 155.5° and nearly 0°, respectively (Figure 10d,e). Here, the surface structure enhanced the intrinsic hydrophobic characteristic of PTFE and rendered it superhydrophobic. Subsequently, an array of micro-through holes was formed by mechanical drilling from the backside of the ablated PTFE sheet. As a result, the drilled sheet displayed high efficiency with respect to oil–water separation. Additionally, it was also effective for the separation of strong acid/alkali substances from oil, indicating the high durability and chemical inertness of PTFE sheets in corrosive environments.
Li et al. employed a FS laser with 104 FS pulse duration and a 1 kHz repetition rate to drill an array of micropores on aluminum foil of 2.4–32 µm diameter and a period of 20–80 µm [70]. Figure 11a,b presents a typical SEM image of the drilled foil, showing that the micropores’ sidewalls are decorated with nanostructures. Although the flat aluminum foil surface is inherently hydrophilic with a water contact angle of 53.9°, the laser-drilled foil became superhydrophilic, showing a water contact angle of 7.8°. As also shown in Figure 11c,d, the oil contact angle of octane and 1,2-dichloroethane was 153.5° and 153.1°, respectively. For the evaluation of the oil–water separation efficiency, oil–water mixtures were poured into a tube that contained a horizontally placed, laser-processed aluminum foil (Figure 12a–c). During the pouring process, water passed through the micropores, while the oil was inhibited due to the superoleophobic property of the foil. For the separation of heavy oil, a tube with a side opening was used, while the irradiated aluminum foil was placed vertically, as shown in Figure 12d–e. The separation process was completed within 31 s. The continuous separation of oil–water mixtures was additionally demonstrated (Figure 13). In that case, the laser-irradiated aluminum foil was modified with 1H,1H,2H,2H-perfluorodecyltriethoxysilane (Figure 13a). Owing to such functionalization treatment, the foil wetting properties changed from superhydrophilic–underwater superoleophobic to superhydrophobic–superoleophilic. Figure 13b shows a schematic representation of the continuous separation process. Both of the membranes (i.e., the laser-irradiated and functionalized one) were placed inside a tube with a side opening. It was observed that the water-selective membrane permitted water to pass through, whereas the oil-selective membrane permitted oil to pass through. The whole process was completed within 28 s. As a result, separation can be achieved by using just the gravity effect, with an efficiency of 99% for both light and heavy oil.
In another approach, a FS laser-processed titanium membrane filter showed high oil–water separation efficiency [69]. In that case, the microholes formed with a spacing of 100–300 µm, using a laser fluence of 3.1–15.5 J/cm2. In particular, the titanium filter prepared with a fluence of 12.4 J/cm2 and 100 µm interspacing showed a remarkable separation efficiency of 99%, with high recyclability. Figure 14 shows a typical SEM image of the titanium membrane filter and the respective energy dispersive x-ray (EDX) analysis of the microholes. Laser ablation leads to the creation of microprotrusions and extensive oxidation of titanium due to oxygen presence in the ambient air.

6. Summary and Outlook

In summary, FS laser surface structuring is a new technology that can be used to create micro- and nanostructures on virtually any type of material. As a consequence of its remarkable ability to control the morphological features at multiple length scales, FS laser processing is a unique tool to tune the wettability of solid surfaces. This capability demonstrates the great potential of FS structuring techniques for oil–water separation applications. Indeed, various approaches to control wettability using FS laser-fabricated surface micro/nanostructure have been explored recently. As a result, superwetting responses, including superhydrophobic–superoleophilic, superhydrophilic–underwater superoleophobic, underwater superoleophobic, and underoil superhydrophobic responses, have been demonstrated for such surfaces and have shown promising results with respect to oil–water separation. This approach has some advantages compared with competitive oil–water separation techniques as far as the durability of the fabricated oil–water separation systems. Specifically, alternative technologies usually employ fragile and low-adhesion fluorinated compounds that lose their superwetting characteristic over a short period of time. On the contrary, FS laser-induced surface structuring can provide surface structures in a single step, without the need for additional chemical coatings. As a result, FS laser-structured filters/membranes have shown promising results of high efficiency, recyclability, and durability with respect to oil–water separation. Oil–water separation by FS laser surface structuring has been realized in two ways, namely meshes decorated with self-organized structures and arrays of microholes created by laser ablation. In both cases, surface structuring may also be followed by a chemical functionalization step. Both meshes and micro-through holes filters have been used for the separation of heavy and light oil/water mixtures.
Although, FS laser surface structures display exceptional oil–water separation efficiency on a laboratory scale, their potential use for separating large volumes of oil–water mixtures in oil spill accidents and organic wastes in industries requires further research. It should be considered that in most of the separation studies, self-prepared oil–water mixtures have been used, which do not perfectly simulate the properties of real oil–water mixtures present in oil leakages and spills. Indeed, oil spills and organic industrial wastes consist of an amalgam of hydrocarbons of different densities, including thick crude oil, emulsions, and surfactants, which could cause fouling and blockage of the micropores present in separation systems. In this context, studies addressing the separation of emulsions and impure organic compounds via FS laser-structured separation systems should be performed. Another study that requires special attention is that of separation at high flux rates, mostly related to the systems used for continuous separation of oil–water mixtures.
Finally, it should be emphasized that the use of FS laser-generated self-organized surface structures for oil–water separation is still considerably limited. To date, only LISR have been used; however, this is not the case for membranes decorated with LISG and LISS structures. Moreover, the use of FS high-pulse energies in laser micromachining via ablation has not been explored yet. The surface structures formed as a result of high-pulse energy laser ablation are expected to provide exceptional results. These studies will also be useful in adapting this technology to large-area membrane systems fabricated in a short period of time.
Considering that oil–water separation via FS laser surface structuring is still in its infancy, significant development is expected on this topic in the near future. This is further supported by the few preliminary but encouraging results on the application of FS laser surface structuring for oil–water separation purposes. It is thus envisaged that FS laser surface structuring will become a unique tool in high-end oil-water separation applications.

Author Contributions

Conceptualization, A.S.A.; Investigation, S.A.K.; Writing-Original Draft Preparation, S.A.K and A.S.A.; Writing-Review and Editing, S.A.K, A.S.A., R.A.G, E.S., Supervision, A.S.A.

Funding

This research was supported by the office of research at the American University of Sharjah.

Acknowledgments

A.S.A. and S.A.K. acknowledge support from the American University of Sharjah.

Conflicts of Interest

The authors declare no conflicts of interest.

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Figure 1. Various two-dimensional (2D) and three-dimensional (3D) structures formed by femtosecond (FS) laser surface structuring under various ablation conditions [32]. Reproduced with permission from [32] line 1–3 Copyrights Royal Society of Chemistry 2015. Line 4 copyrights Elsevier 2014.
Figure 1. Various two-dimensional (2D) and three-dimensional (3D) structures formed by femtosecond (FS) laser surface structuring under various ablation conditions [32]. Reproduced with permission from [32] line 1–3 Copyrights Royal Society of Chemistry 2015. Line 4 copyrights Elsevier 2014.
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Figure 2. Typical setup used for femtosecond laser surface structuring and microfabrication.
Figure 2. Typical setup used for femtosecond laser surface structuring and microfabrication.
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Figure 3. Different types of femtosecond (FS) laser-induced self-organized periodic surface structures (LIPSS) [2].
Figure 3. Different types of femtosecond (FS) laser-induced self-organized periodic surface structures (LIPSS) [2].
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Figure 4. Various LIPSS types formed by FS laser pulses of different polarization: (a) Grating-like Laser-induced surface ripples (LISR) formation fabricated with linear polarization; (b) rhomboidal multi-directional surface structures produced by radial polarization; and (c) columnar structures fabricated by circular polarization. The corresponding fast Fourier transform (FFT) diagrams are also shown, revealing the different spatial frequencies included in each structure [30].
Figure 4. Various LIPSS types formed by FS laser pulses of different polarization: (a) Grating-like Laser-induced surface ripples (LISR) formation fabricated with linear polarization; (b) rhomboidal multi-directional surface structures produced by radial polarization; and (c) columnar structures fabricated by circular polarization. The corresponding fast Fourier transform (FFT) diagrams are also shown, revealing the different spatial frequencies included in each structure [30].
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Figure 5. (a–d) Titanium sample irradiated with F = 0.35 J/cm2 (a) 1 laser shot, (b) 40 laser shots, (c) 100 laser shots, and (d) 200 laser shots [21]. Reproduced with permission from [21] Elsevier 2007. (e,f) Black silicon surfaces obtained upon FS laser processing in air and SF6 ambient conditions, respectively [2].
Figure 5. (a–d) Titanium sample irradiated with F = 0.35 J/cm2 (a) 1 laser shot, (b) 40 laser shots, (c) 100 laser shots, and (d) 200 laser shots [21]. Reproduced with permission from [21] Elsevier 2007. (e,f) Black silicon surfaces obtained upon FS laser processing in air and SF6 ambient conditions, respectively [2].
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Figure 6. Different wetting states of water and oil droplets. (a) Young state of a droplet on a flat surface; (b) definition of the sliding angle (SA) or roll-off angle; (c) Wenzel state where the liquid completely wets the surface structures; (d) transitional or partial wetting state; (e) Cassie–Baxter state, where the droplet sits on the microstructures and air is trapped beneath it; and (f) oil droplet underwater in the Cassie–Baxter state.
Figure 6. Different wetting states of water and oil droplets. (a) Young state of a droplet on a flat surface; (b) definition of the sliding angle (SA) or roll-off angle; (c) Wenzel state where the liquid completely wets the surface structures; (d) transitional or partial wetting state; (e) Cassie–Baxter state, where the droplet sits on the microstructures and air is trapped beneath it; and (f) oil droplet underwater in the Cassie–Baxter state.
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Figure 7. (a,b) SEM image of FS laser-structured Janus wire mesh. (c) Laser-structured fluorosilane-modified mesh (580 mW, 7.39 × 106 mJ/cm2) at different magnifications. LISR with a period of 900 nm at fluorosilane-modified mesh. (d) Elemental map of fluorosilane-modified mesh showing the presence of fluorine and silicon. (e,f) Laser-structured GO-modified mesh (100 mW, 12.74 × 105 mJ/cm2) at different magnifications. (g) LISR covered with GO wrinkles. (h) Elemental map of GO-modified mesh showing the high presence of oxygen and carbon [66]. Reproduced with permission from [66] Royal Society of Chemistry 2017.
Figure 7. (a,b) SEM image of FS laser-structured Janus wire mesh. (c) Laser-structured fluorosilane-modified mesh (580 mW, 7.39 × 106 mJ/cm2) at different magnifications. LISR with a period of 900 nm at fluorosilane-modified mesh. (d) Elemental map of fluorosilane-modified mesh showing the presence of fluorine and silicon. (e,f) Laser-structured GO-modified mesh (100 mW, 12.74 × 105 mJ/cm2) at different magnifications. (g) LISR covered with GO wrinkles. (h) Elemental map of GO-modified mesh showing the high presence of oxygen and carbon [66]. Reproduced with permission from [66] Royal Society of Chemistry 2017.
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Figure 8. (a) Optical and (b,c) SEM images of stainless-steel mesh before and after FS laser treatment. (d,e) SEM images of LISR present on the FS laser-irradiated mesh, at different magnifications; (f,g) chemical composition analysis of the pristine and the laser-treated stainless-steel mesh [67]. Reproduced with permission from [67] Royal Society of Chemistry 2017.
Figure 8. (a) Optical and (b,c) SEM images of stainless-steel mesh before and after FS laser treatment. (d,e) SEM images of LISR present on the FS laser-irradiated mesh, at different magnifications; (f,g) chemical composition analysis of the pristine and the laser-treated stainless-steel mesh [67]. Reproduced with permission from [67] Royal Society of Chemistry 2017.
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Figure 9. Oil–water separation with a superhydrophilic–underwater superoleophobic FS laser-treated mesh. Contrary to water, oil is repelled, while both the liquids are collected in separate containers [67]. Reproduced with permission from [67] Royal Society of Chemistry.
Figure 9. Oil–water separation with a superhydrophilic–underwater superoleophobic FS laser-treated mesh. Contrary to water, oil is repelled, while both the liquids are collected in separate containers [67]. Reproduced with permission from [67] Royal Society of Chemistry.
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Figure 10. (a–c) SEM of FS laser surface structures on the PTFE surface at different magnifications. (d) Image of a water droplet and oil droplet on the PTFE structured surface. (e) Water contact angle measurement of the PTFE laser-structured surface [68]. Reproduced with permission from Elsevier 2016.
Figure 10. (a–c) SEM of FS laser surface structures on the PTFE surface at different magnifications. (d) Image of a water droplet and oil droplet on the PTFE structured surface. (e) Water contact angle measurement of the PTFE laser-structured surface [68]. Reproduced with permission from Elsevier 2016.
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Figure 11. (a) SEM image of the micropores drilled in ultrathin aluminum foil by FS laser ablation; the inset shows that light can pass through the micropores’ array. (b) Magnified image of the treated foil showing that the rim of the pores is decorated with microstructures; (c) underwater contact angle of a light oil (C8H18) droplet on the laser-treated aluminum foil; and (d) underwater contact angle of a heavy oil (C2H4Cl2) droplet on the laser-treated aluminum foil [70]. OCA: oil contact angle. Reproduced with permission from [70] Royal Society of Chemistry 2016.
Figure 11. (a) SEM image of the micropores drilled in ultrathin aluminum foil by FS laser ablation; the inset shows that light can pass through the micropores’ array. (b) Magnified image of the treated foil showing that the rim of the pores is decorated with microstructures; (c) underwater contact angle of a light oil (C8H18) droplet on the laser-treated aluminum foil; and (d) underwater contact angle of a heavy oil (C2H4Cl2) droplet on the laser-treated aluminum foil [70]. OCA: oil contact angle. Reproduced with permission from [70] Royal Society of Chemistry 2016.
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Figure 12. (a) Oil–water mixture of heavy and light oil. (b) Schematic of the light oil–water separation process; (c) oil–water separation was completed within 13 s in the case of the octane light oil. (d) Tube with side opening and schematic of the heavy oil–water separation process; (e) the heavy oil–water separation process was completed within 31 s [70]. Reproduced with permission from [70] Royal Society of Chemistry 2016.
Figure 12. (a) Oil–water mixture of heavy and light oil. (b) Schematic of the light oil–water separation process; (c) oil–water separation was completed within 13 s in the case of the octane light oil. (d) Tube with side opening and schematic of the heavy oil–water separation process; (e) the heavy oil–water separation process was completed within 31 s [70]. Reproduced with permission from [70] Royal Society of Chemistry 2016.
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Figure 13. (a) Schematic of the modification of a FS laser-drilled aluminum foil with 1H,1H,2H,2H-perfluorodecyltriethoxysilane. Following this process, the water contact angle (WCA) turned from superhydrophilic (WCA ~5.1°) to superhydrophobic (WCA ~154.4°); (b) schematic illustration of the continuous separation of an oil–water mixture by superhydrophobic and superhydrophilic foil; (c) the continuous separation of an oil–water mixture, which was completed in 28 s [70]. WCA: water contact angle. Reproduced with permission from [70] Royal Society of Chemistry 2016.
Figure 13. (a) Schematic of the modification of a FS laser-drilled aluminum foil with 1H,1H,2H,2H-perfluorodecyltriethoxysilane. Following this process, the water contact angle (WCA) turned from superhydrophilic (WCA ~5.1°) to superhydrophobic (WCA ~154.4°); (b) schematic illustration of the continuous separation of an oil–water mixture by superhydrophobic and superhydrophilic foil; (c) the continuous separation of an oil–water mixture, which was completed in 28 s [70]. WCA: water contact angle. Reproduced with permission from [70] Royal Society of Chemistry 2016.
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Figure 14. (a–d) SEM image of a FS laser-fabricated titanium membrane filter showing the presence of microprotrusions at the periphery of the microholes; (e,f) EDX analysis of the pristine and FS laser-treated titanium foil [69].
Figure 14. (a–d) SEM image of a FS laser-fabricated titanium membrane filter showing the presence of microprotrusions at the periphery of the microholes; (e,f) EDX analysis of the pristine and FS laser-treated titanium foil [69].
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Table
Table 1. Oil–water separation filters/meshes realized by FS laser fabrication.
Table 1. Oil–water separation filters/meshes realized by FS laser fabrication.
MaterialLaser StructuresFabrication ParametersChemical TreatmentWettability CharacteristicOil SeparatedRef.
FS Laser-Structured Meshes
Janus mesh (side 1)LISR580 mW, 7.39 × 106 mJ/cm21H,1H,2H,2H-perfluorodecyltriethoxysilaneSuperhydrophobic–superoleophilicBean oil, n-heptane, methyl benzene[66]
Janus mesh (side 2)--Graphene oxidesuperhydrophilic–underwater superoleophobicPerchloromethane, trichloromethane.
Stainless steelLISRλ = 1030 nm, 250 FS, 75 kHz-superhydrophilic–underwater superoleophobicEdible oil, diesel, crude oil, hexadecane, 1,2-dichloroethane.[67]
FS Laser-Fabricated Arrays of Micro-Through Holes
PTFE-λ = 800 nm, 50 FS, 1 kHz,-superhydrophobic–superoleophilicpetroleum ether, acid/base (HCl and KOH) solution,[68]
Titanium-λ = 800 nm, 50 FS, 1 kHz, 3.1–15.5 J/cm2-Superhydrophilic underwater–superoleophobicpetroleum ether, heptane, hexane, gasoline, crude oil, soybean, silicon oil[69]
Aluminum-λ = 800 nm,104 FS, 1 kHz, 4–5 pulses/hole1H,1H,2H,2H-perfluorodecyltriethoxysilane (PFDTES)superhydrophilic underwater–superoleophobic
superhydrophobic–superoleophilic		Octane, 1,2-dichloroethane[70]
LISR: laser-induced surface ripples, PTFE: polytetrafluoroethylene.

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MDPI and ACS Style

Alnaser, A.S.; Khan, S.A.; Ganeev, R.A.; Stratakis, E. Recent Advances in Femtosecond Laser-Induced Surface Structuring for Oil–Water Separation. Appl. Sci. 2019, 9, 1554. https://doi.org/10.3390/app9081554

AMA Style

Alnaser AS, Khan SA, Ganeev RA, Stratakis E. Recent Advances in Femtosecond Laser-Induced Surface Structuring for Oil–Water Separation. Applied Sciences. 2019; 9(8):1554. https://doi.org/10.3390/app9081554

Chicago/Turabian Style

Alnaser, Ali Sami, Sharjeel Ahmed Khan, Rashid Ashirovich Ganeev, and Emmanuel Stratakis. 2019. "Recent Advances in Femtosecond Laser-Induced Surface Structuring for Oil–Water Separation" Applied Sciences 9, no. 8: 1554. https://doi.org/10.3390/app9081554

APA Style

Alnaser, A. S., Khan, S. A., Ganeev, R. A., & Stratakis, E. (2019). Recent Advances in Femtosecond Laser-Induced Surface Structuring for Oil–Water Separation. Applied Sciences, 9(8), 1554. https://doi.org/10.3390/app9081554

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