Photoresponsive titania surfaces are of great interest due to their unique wettability change upon ultraviolet light illumination. However, their applications are often limited either by the inability to respond to visible light or the need for special treatment to recover the original wettability. Sensitizing TiO2 surfaces with visible light-absorbing materials has been utilized in photovoltaic applications. Here we demonstrate that a dye-sensitized TiO2 surface can selectively change the wettability towards contacting liquids upon visible light illumination due to a photo-induced voltage across the liquid and the underlying surface. The photo-induced wettability change of our surfaces enables external manipulation of liquid droplet motion upon illumination. We show demulsification of surfactant-stabilized brine-in-oil emulsions via coalescence of brine droplets on our dye-sensitized TiO2 surface upon visible light illumination. We anticipate that our surfaces will have a wide range of applications including microfluidic devices with customizable wettability, solar-driven oil–water clean-up and demulsification technologies.
Photo-responsive surfaces are of great interest due to the wettability change induced upon exposure to incident light1,2,3. One way to achieve photo-induced wettability change is utilizing photochromic molecules that display reversible transformations upon illumination between two chemical states having different dipole moments or polar moieties4,5,6. However, such organic photochromic molecules typically exhibit low contact angle change upon contact with liquid droplets4,6,7,8. Recently, it has been reported that photo-generated charge carriers (electron–hole pairs) can change the capacitance of semiconducting silicon dioxide which in turn change the wettability toward a contacting liquid9,10. The wettability change is amplified when the semiconductor is subject to an externally applied voltage along with light illumination9,10.
Photo-responsive titania (TiO2) surfaces have demonstrated wettability change upon exposure to ultraviolet light1,3. A great deal of work has been devoted to elucidating the origin of the well-documented unique ultraviolet light-induced wettability change on TiO2 surfaces2,11,12,13. Although this continues to remain an active area of research, it is widely accepted that photo-generated electrons and holes change the surface chemistry so that it is favourable for contacting liquids to spread either by photocatalytic oxidation of surface adsorbed organic species11,12 or by the increase of hydroxyl species due to dissociative water adsorption2,13.
Photo-driven manipulation of liquid motion on a TiO2 surface is highly attractive because it would eliminate any need for either direct electrical contact with liquids or complex electronic circuitry14,15. However, their practical applications are often limited either by the inability to respond to the visible light spectrum of natural sunlight16,17 or by the slow kinetics and the need for special environments (that is, storage in dark or heat) to recover the original wetting state18,19.
The strategy of sensitizing TiO2 surfaces with dopants and visible light-absorbing materials (for example, organic dyes) has been utilized in photovoltaics to efficiently absorb solar radiation and convert it to electrical energy20,21. Imbibition of a liquid dye or adsorption of dye to a TiO2 surface is an alternative approach for generating charge carriers upon light illumination20,21,22. On a dye-sensitized TiO2 surface, the optical absorption and charge-generating functions are achieved by excitation of dye and subsequent injection of charge carriers (for example, electrons) into the conduction band of TiO2 (refs 22, 23, 24). The light absorption behaviour of a dye-sensitized TiO2 surface can be readily tuned by careful consideration of the energy levels of the selected dye. Ruthenium (II) polypyridyl complexes have received particular interest due to their wide absorption range from the visible to the near-infrared regime and high stability in the oxidized state25. Furthermore, introduction of a textured roughness or porosity to the TiO2 surface can dramatically increase the light absorption efficiency due to an increased specific surface area providing capillary stabilization of a surface adsorbed liquid film in which a large number of dye molecules can be directly adsorbed20,21. Consequently, dye-sensitization may provide a versatile tool to tune the wettability of TiO2 surfaces under visible light illumination.
In this work, we demonstrate that a dye-sensitized TiO2 surface—fabricated using straightforward dip-coating method—can be engineered to have its wettability state optically modulated upon illumination by visible light. We show that this wettability change arises due to the electric potential difference established between the surface and the liquid upon incident illumination. A systematic study of the relationship between the energy levels of the dye and the contacting liquid reveals that the highest occupied molecular orbital (HOMO) energy level of the dye and the reduction potential of the liquid govern the ensuing wetting behaviours. Utilizing this photo-induced wetting of our dye-sensitized TiO2 surface we demonstrate light-guided manipulation of liquid droplet motion along the surface. Furthermore, we show demulsification of surfactant-stabilized brine-in-oil emulsion via interfacial coalescence of brine droplets under visible light illumination. Such surfaces thus offer a wide range of potential applications including optically driven, microfluidic devices with customizable wettability5,26 and continuous solar-driven self-cleaning and oil–water separation technologies27,28.
Wetting behaviours of liquids on an N3 dye-sensitized TiO2
We fabricated an N3 dye-sensitized TiO2 surface. A thin, nanostructured and highly porous TiO2 surface is prepared by layer-by-layer (LBL) deposition of negatively charged TiO2 nanoparticles (average diameter ≈20 nm) and positively charged poly(allylamine hydrochloride) (PAH) on an indium tin oxide (ITO)-coated glass slide followed by calcination (see Methods). A scanning electron microscopy image (see inset (i) in Fig. 1a) shows that the surface is highly porous with a large specific surface area. The ratio of the total surface area per unit projected area is estimated to be 56 (see Supplementary Note 1). The resulting porous TiO2 surface is subsequently dip-coated in N3 dye solution. N3 dye molecules chemisorb to the surface via carboxylate groups29,30. Adsorption of N3 dye molecules leads to a deep brown coloration of the surface (see inset (ii) in Fig. 1a). We measured the visible light absorption spectra of an N3 dye-sensitized TiO2 surface and, as shown in Fig. 1a, our surface absorbs a broad range of the incident visible spectrum (390 nm≤λ≤700 nm). In contrast, an unsensitized LBL-deposited TiO2 nanostructured surface displays negligible absorption in the visible regime due to the wide band gap energy of the TiO2 particles (≈3.2 eV)31.
To study the photo-induced wettability change of our N3 dye-sensitized TiO2 surface, we measured the evolution in the contact angles in situ for three liquid droplets: deionized (DI) water, potassium iodide (KI, 10 wt% in water) and potassium chloride (KCl, 10 wt% in water). In situ contact angle measurements were conducted under oil (for example, dodecane) environment to minimize evaporation of a droplet due to the heat generated from the light source (see inset (i) in Fig. 1b and Methods) and to simulate the condition expected in oil–water separation operation32,33,34,35. The visible light source with intensity (I=145 mW cm−2) is projected from above the surface to minimize intensity loss along the light transmission path. Figure 1b shows the evolution in the macroscopic contact angles (θ*) for DI water, KI and KCl droplets as a function of illumination time. The equilibrium contact angles for DI water and KCl remain almost constant during illumination ( and where ), while those for KI decrease progressively from with increasing illumination time before finally approaching (see Fig. 1b). After it reaches 77°, the contact angle remains unchanged. Similar contact angle saturation is also typically observed in conventional electrowetting-on-dielectric applications36. Very similar contact angle changes were also observed on a thicker N3 dye-sensitized TiO2 film prepared with 45 bilayers of TiO2 and PAH. We also observed that the negligible wettability change for KCl was independent of concentration (see Supplementary Table 1) while KI droplets with higher ionic concentration exhibited rapid decrease in contact angles (see Supplementary Fig. 1 and Supplementary Note 2). Note that unlike the conventional electrowetting (or photoelectrowetting) where the contact angle change is effected within milliseconds upon (high) voltage application37, our N3 dye-sensitized TiO2 surface exhibits a wettability change for KI droplet over tens of minutes. However, the switchability does not require application of large voltages, and can be effected using droplets on surfaces that are immersed in alkanes or other low surface tension organic liquids. The expected application areas will thus be very different to conventional electrowetting devices. Our selective photo-induced wetting response of KI over KCl (or DI water) is further exemplified by considering multiple wetting cycles as shown in Fig. 1c. The contact angles for fresh droplets of KI placed at a fixed location on the surface cycles between and under repeated illumination, while that for KCl remains almost constant. Unlike an unsensitized, as-fabricated TiO2 surface, X-ray photoelectron spectroscopy analysis of our N3 dye-sensitized TiO2 surface clearly indicates that the surface chemistry remains unaffected after multiple cycles of wetting under visible light illumination (see Supplementary Fig. 2 and Supplementary Note 3).
The origin of the photo-induced wettability change
On dye-sensitized TiO2 surfaces, photo-generated electrons from incident visible light illumination are injected and travel through the nanoporous TiO2 network23,24. We can anticipate that this electron transfer results in the generation of an electric potential difference between the surface and the contacting liquid that can then induce electrowetting effects in liquid droplets on the surface. To understand this further, we first consider the physicochemical origin of a photo-induced electric potential difference under light illumination.
Figure 2a shows a schematic and energy diagram of an N3 dye-sensitized TiO2 surface contacting a KI droplet. After electron transfer upon illumination, a region over which the charge distribution differs from the bulk is produced. This corresponds to the electrolytic double layer and the accumulation layer at the contacting KI and TiO2, respectively22. Consequently, an electric potential difference (that is, a measurable voltage) is generated between the contacting KI droplet and the underlying substrate. The oxidized dye (D+) can be subsequently reduced by accepting an electron from the reducing agent (that is, the iodide, I−) in the KI through the chemical reaction (a process known as regeneration)38,39. An alternative pathway for reducing the oxidized dye is by recombining with an electron in the TiO2 (that is, the process of recombination)40,41. While the regeneration is more favourable and orders of magnitude faster42,43, the recombination also plays an important role in dye reduction process, especially under open-circuit conditions44,45.
To validate our hypothesis, we measured the in situ voltage across the contacting liquids and the N3 dye-sensitized TiO2 surface while illuminating with visible light (see Fig. 2b). Immediately after the onset of illumination, a potential difference VKI, t=0 ≈0.42 V is observed between the KI and the lower ITO electrode. The voltage decreases gradually with increasing illumination time and eventually reaches zero after t≈45 min. Similar to photoelectrowetting9,46 in which the voltage along with optically generated charge carriers leads to wetting, the photo-induced voltage causes spreading of the KI droplet on our N3 dye-sensitized TiO2 surface. The gradual decrease in the measured voltage can be explained by considering electrolytic double layer as a capacitor (C) and the underlying TiO2 film as a resistor (R). Thus, the KI droplet and the TiO2 film can be considered as an RC circuit connected in series. When the capacitor in an RC circuit is discharged, the voltage V(t) is given by
where Vo, τd and α denote the voltage at t=0, the relaxation time constant and the fractional derivative order, respectively. Note that equation (1) characterizes a fractional RC circuit in which the capacitor (or a resistor) is imperfect47. For example, the electrolytic double layer here may be a leaky capacitor due to the defects present on the surface of the nanoparticles. Our measured voltages across the KI and ITO (see Fig. 2b) match well with equation (1) with τd=130 s and α=0.42 (see Supplementary Note 4). Furthermore, we observed that changes in the contact angle halt instantaneously and the droplet shape remains unchanged when the illumination is turned off (see Supplementary Fig. 3 and Supplementary Note 5).
Unlike the gradual decrease in voltage between the KI droplet and the surface during optical illumination, we observed a rapid decrease in the voltage between a KCl droplet and the surface after the onset of illumination (see Fig. 2b). Rapid decrease in the voltage highlights the importance of the dye reduction process in photo-induced voltage generation. As the reduction potential of iodide (I−, Ered, I−=0.53 V versus normal hydrogen electrode (NHE))48 is above (that is, less positive than) the HOMO energy level of N3 dye (EHOMO, N3=1.0 V versus NHE)49, it presents a driving force to reduce the oxidized dye. As a consequence, an N3 dye-sensitized TiO2 surface contacting a KI droplet can maintain a prolonged voltage difference by suppressing the recombination process. In contrast, chloride (Cl−, Ered, Cl−=1.36 V versus NHE)48 cannot effectively reduce the oxidized N3 dye due to its higher reduction potential resulting in a dominant recombination process.
To probe our hypothesis that suppressing the recombination process leads to prolonged photo-induced voltage generation, and subsequently extension of the wetting (that is, a larger change in contact angles), we fabricated an electrically grounded N3 dye-sensitized TiO2 surface (see inset in Fig. 2c). In contrast to the previous surface where photo-generated electrons continue to accumulate and participate in the recombination process, the electrically grounded surface minimizes electron accumulation. Figure 2c shows an enhanced decrease in macroscopic contact angles for KI and KCl droplets on the electrically grounded N3 dye-sensitized TiO2 surface after 120 min of illumination. We anticipate that this is a direct consequence of the suppression of the recombination process.
Photo-induced wetting on various dyes-sensitized TiO2
These findings described above provide us with design parameters to systematically manipulate the wettability of dye-sensitized TiO2 surfaces towards different contacting liquids in response to visible light illumination. For effective wetting of specific liquids, it is preferential to regenerate the oxidized dye by a reducing agent within the contacting liquid (see Fig. 2a). This often requires careful consideration of the energy levels of the dye and different contacting liquids. As is well documented in the dye-sensitized solar cell literature23,24, effective dye regeneration is typically achieved by using electrolytes that possess a reduction potential that is less positive than the HOMO energy level of dye. This enables us to create a design chart for photo-induced wetting of contacting liquids on a dye-sensitized TiO2 surface. Figure 3a shows an energy diagram of various dyes and electrolytes. Here we chose D149 dye50 and Chlorin dye51 as sensitizers (see Methods). Similar to our N3 dye-sensitized TiO2 surface, a D149 dye-sensitized TiO2 and a Chlorin dye-sensitized TiO2 absorb across a broad range of the visible light spectrum (see Supplementary Fig. 4 and Supplementary Note 6). As their lowest unoccupied molecular orbital (LUMO) energy levels are above (that is, less positive than) the conduction band of TiO2, efficient electron transfer can be achieved50,51,52. However, subsequent regeneration of the oxidized dyes by various electrolytes will be selective due to their different HOMO energy levels (EHOMO, D149=1.14 V versus NHE50 and EHOMO, Chlorin=1.72 V versus NHE51) with respect to the reduction potentials of various electrolytes. Along with KI and KCl, we utilized potassium thiosulfate (K2S2O3, 10 wt% in water, Ered, K2S2O3=0.08 V versus NHE)48 and potassium bromide (KBr, 10 wt% in water, Ered, KBr=1.09 V versus NHE)48 as contacting liquids. In situ photo-induced voltage measurements of a D149 dye-sensitized TiO2 and a Chlorin dye-sensitized TiO2 in contact with droplets of various electrolytes clearly indicate that a prolonged voltage difference across the surface and the contacting liquid droplet is achieved when EHOMO, dye>Ered, liquid (see Supplementary Fig. 5 and Supplementary Note 7). Supplementary Table 2 lists the values of τd and α found in the voltage predictions using our RC circuit model. Figure 3b shows the evolution in the macroscopic contact angles for K2S2O3, KI, KBr and KCl droplets on a D149 dye-sensitized TiO2 surface under illumination. Contacting liquids with a lower reduction potential (that is, less positive) than EHOMO, D149 (for example, K2S2O3, KI and KBr, see also Fig. 3a) spread on the surface, while a droplet of KCl exhibits a negligible contact angle decrease. In contrast, we observed a decrease in the macroscopic contact angles for all contacting liquids on a Chlorin dye-sensitized TiO2 surface under visible light illumination (see Fig. 3c). This is a direct consequence of the effective dye-regeneration process with all contacting liquids as a result of the very high EHOMO of Chlorin dye51,52. Selective wetting behaviours of K2S2O3 (or KI) over KBr (or KCl) on an N3 dye-sensitized TiO2 surface is also observed (see Supplementary Fig. 6 and Supplementary Note 8). To the best of our knowledge, this is the first-ever systematic demonstration of visible light-induced wetting of contacting liquid droplet on dye-sensitized TiO2 surfaces.
Manipulating liquid droplet on a Chlorin dye-sensitized TiO2
Our ability to photo-induce the selective wetting of contacting liquids on a dye-sensitized TiO2 surface provides a versatile tool to manipulate liquid motion. Figure 4a shows visible light guided movement of a sodium chloride (NaCl; 10 wt% in water) droplet on a patterned dye-sensitized TiO2 surface submerged in dodecane. Our patterned surface consists of a thin channel of Chlorin dye-sensitized LBL-assembled nanoporous TiO2 surrounded by a hydrophobic background (see Methods). A droplet of NaCl is placed on the channel, and white light is focused on one edge of the droplet (see Fig. 4a (i)). The contact angle at the interface between the liquid and the illuminated surface decreases while the other side remains pinned. Consequently, the droplet’s centre of mass moves towards the illuminated edge (see Fig. 4a (ii)). Further illumination leads to an elongation of the droplet shape (see Fig. 4a (iii)). Supplementary Movie 1 demonstrates the photo-induced anisotropic wetting (that is, progressive spreading in one direction while the other side remains pinned) of a NaCl droplet on a Chlorin dye-sensitized TiO2 surface. Sequential snapshot images are also shown in Fig. 4a (iv)–(vi). This anisotropic wetting behaviour under focused optical illumination allows for coalescence of multiple aqueous droplets that are initially pinned on the surface. Figure 4b shows sequential photographs of the coalescence of multiple NaCl droplets on a Chlorin dye-sensitized TiO2 surface submerged in dodecane. By shining visible light at various locations between the droplets we can photo-induce coalescence of all droplets resulting in a single continuous NaCl aqueous layer on the surface.
Demulsification of brine-in-oil emulsions
This photo-induced coalescence process is an ideal candidate to substitute for conventional electrostatic coalescence technique employed in demulsification32,33,34 (that is, the conversion of an oil–water emulsion into two separate oil-free and water-free phases), especially for mixtures with high salt concentration (for example, brine–oil emulsions) that are typically generated in enhanced oil-recovery operations. The demulsification of brine–oil emulsions using our photo-induced coalescence is highly desirable because conductive emulsions resulting from ionized salts create a current path upon application of an external electric field that hinders generation of induced dipole moments53. Here we demonstrate demulsification of a brine–oil emulsion utilizing photo-induced coalescence of water droplets containing salts on a dye-sensitized TiO2 surface. Figure 5a,b show demulsification of a brine (10 wt% NaCl in water)-in-dodecane emulsion stabilized by 0.1 wt% of Span80 surfactant (see Methods). The demulsification apparatus consists of a stainless steel membrane (pore size ≈2 μm) coated with Chlorin dye-sensitized TiO2 nanostructured film sandwiched between the two vertical glass tubes (see Fig. 5a). The emulsion is added to the upper tube and immediately visible light is illuminated on the membrane surface. Within minutes of illumination, the brine-in-dodecane emulsion demulsifies into brine-rich and dodecane-rich phases (see Fig. 5b). Similar to photo-induced coalescence of NaCl droplets (see Fig. 4b), brine droplets that contact the Chlorin dye-sensitized TiO2 mesh surface spread and coalesce with other droplets under white light illumination. Figure 5c shows a schematic illustrating our photo-induced demulsification of brine–oil emulsion. Figure 5d shows the brine droplet number size distribution of the dodecane-rich retentate after 4 min of demulsification. By comparing with the feed emulsion, it is evident that nearly all brine droplets above 25 μm (that is, >99.9 vol% of brine) are removed by photo-induced coalescence. Supplementary Movie 2 demonstrates the demulsification of a brine-in-oil emulsion using photo-induced coalescence of brine droplets on Chlorin dye-sensitized TiO2 mesh surface.
In summary, we have demonstrated that dye-sensitized nanoporous TiO2 surfaces can selectively change the wettability towards contacting liquids upon visible light illumination due to a photo-induced voltage difference across the liquid and the surface. We have also shown that the HOMO energy level of the selected dye and the reduction potential of the contacting liquid droplet phase govern the effective dynamics of the photo-induced voltage difference. The photo-induced wettability change of a dye-sensitized TiO2 surface enables external manipulation of liquid droplet motion across a surface upon visible light illumination. We also demonstrated spontaneous demulsification and separation of surfactant-stabilized brine-in-oil emulsion using photo-induced coalescence of brine droplets on a dye-sensitized TiO2 surface. We anticipate that such abilities to remotely activate and control the wettability states of surfaces through optical illumination will enable new microfluidic separation technologies as well as result in new sunlight-driven oil–water clean-up and demulsification approaches.
Fabrication of thin nanostructured TiO2 surfaces
A thin, nanostructured TiO2 surface was fabricated using LBL deposition either on an ITO-coated glass slide (Sigma Aldrich, surface resistivity=8–12 Ω sq−1) or stainless steel mesh (TWP Inc., pore size ≈2 μm) substrates. First, the substrates were thoroughly rinsed with isopropyl alcohol and DI water followed by drying with nitrogen gas. The cleaned substrates were sequentially dip-coated in PAH (Sigma Aldrich, average molecular weight=15,000 g mol−1) aqueous solution (1 mg ml−1, pH=7.5) and TiO2 nanoparticle (Svaya Nanotechnology, average diameter ≈20 nm) aqueous dispersion (0.03 wt%, pH=9.0). After depositing desired number of bilayers (30 or 45 bilayers) of PAH and TiO2, the substrates were calcined at 400 °C for 2 h to remove PAH from the surface. A scanning electron microscopy image shows that the surface is highly porous (see inset (i) in Fig. 1a).
Fabrication of dye-sensitized TiO2 surfaces
Solutions (0.3 mM) of N3 dye (Sigma Aldrich), D149 dye (Sigma Aldrich) and Chlorin dye (Frontier Scientific) were prepared in anhydrous ethanol (Fischer Scientific). Note that N3 dye, D149 dye and Chlorin dye denote cis-bis(isothiocyanato) bis(2,2′-bipyridyl-4,4′-dicarboxylato ruthenium (II), 5-[[4-[4-(2,2-diphenylethenyl)phenyl]-1,2,3,3a,4,8b-hexahydrocyclopent[b]indol-7 yl]methylene]-2-(3-ethyl-4-oxo-2-thioxo-5-thiazolidinylidene)-4-oxo-3-thiazolidineacetic acid and 13-carboxy-17-(2-carboxyethyl)-15-carboxymethyl-17,18-trans-dihydro-3-vinyl-8-ethyl-2,7,12,18 tetramethylporphyrin, respectively. Small pieces of substrates with TiO2 surface were dip-coated in the desired solution for 12 h followed by thorough rinsing with ethanol to remove any residual dye molecules from the surface. The substrates were then dried with nitrogen gas.
In situ contact angle measurements
A small volume (=4 μl) of ionic aqueous droplet was placed onto a dye-sensitized TiO2 surface submerged in dodecane. Visible light (MI 150, Edmund Optics) was irradiated from the top of the droplet. Note that the intensity of the light was constant (I=145 mW cm−2) in all measurements. The contact angle measurements were conducted using a Ramé–Hart 590-F1 goniometer.
Fabrication of a patterned dye-sensitized TiO2 surface
A glass slide was masked in a channel (5 mm wide × 15 mm long) by Kapton polyimide adhesive tape (ULINE) by manual application. A TiO2 film was prepared on the unmasked region using LBL deposition followed by calcination as described above. Subsequently, the substrate was dip-coated in a Chlorin dye solution for 12 h to obtain a Chlorin dye-sensitized TiO2 channel. The channel was then masked by attaching a crosslinked polydimethylsiloxane (x-PDMS) film. The substrate was treated with heptadecafluoro-1,1,2,2-tetrahydrodecyl trichlorosilane (Gelest) by vapour phase deposition at 90 °C for 1 h to obtain hydrophobic background.
Demulsification of a brine-in-dodecane emulsion
A brine-in-dodecane emulsion (30:70 v:v) was prepared by mixing water with 10 wt% NaCl and dodecane using a stir bar at 1,000 r.p.m. The concentration of Span80 surfactant was 0.1 wt% to dodecane phase. The emulsion is added onto a stainless steel mesh coated with a Chlorin dye-sensitized TiO2 film that is sandwiched between the two vertical glass tubes. After addition of emulsion, visible light is illuminated onto the mesh surface to induce coalescence of brine droplets.
The authors declare that the data supporting the findings of this study are available within the article and its Supplementary Information files.
How to cite this article: Kwon, G. et al. Visible light guided manipulation of liquid wettability on photoresponsive surfaces. Nat. Commun. 8, 14968 doi: 10.1038/ncomms14968 (2017).
Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Wang, R. et al. Light-induced amphiphilic surfaces. Nature 388, 431–432 (1997).
Sun, R. D., Nakajima, A., Fujishima, A., Watanabe, T. & Hashimoto, K. Photoinduced surface wettability conversion of ZnO and TiO2 thin films. J. Phys. Chem. B 105, 1984–1990 (2001).
Wang, R. et al. Photogeneration of highly amphiphilic TiO2 surfaces. Adv. Mater. 10, 135–138 (1998).
Vlassiouk, I., Park, C. D., Vail, S. A., Gust, D. & Smirnov, S. Control of nanopore wetting by a photochromic spiropyran: a light-controlled valve and electrical switch. Nano Lett. 6, 1013–1017 (2006).
Ichimura, K., Oh, S. K. & Nakagawa, M. Light-driven motion of liquids on a photoresponsive surface. Science 288, 1624–1626 (2000).
Rosario, R. et al. Photon-modulated wettability changes on spiropyran-coated surfaces. Langmuir 18, 8062–8069 (2002).
Moller, G., Harke, M., Motschmann, H. & Prescher, D. Controlling microdroplet formation by light. Langmuir 14, 4955–4957 (1998).
Matsumoto, M. et al. Reversible light-induced morphological change in Langmuir-Blodgett films. J. Am. Chem. Soc. 120, 1479–1484 (1998).
Arscott, S. Moving liquids with light: photoelectrowetting on semiconductors. Sci. Rep. 1, 184 (2011).
Gaudet, M. & Arscott, S. Optical actuation of microelectromechanical systems using photoelectrowetting. Appl. Phys. Lett. 100, 224103 (2012).
Ohtsu, N., Masahashi, N., Mizukoshi, Y. & Wagatsuma, K. Hydrocarbon decomposition on a hydrophilic TiO2 surface by UV irradiation: spectral and quantitative analysis using in-situ XPS technique. Langmuir 25, 11586–11591 (2009).
Zubkov, T. et al. Ultraviolet light-induced hydrophilicity effect on TiO2(110)(1 × 1). Dominant role of the photooxidation of adsorbed hydrocarbons causing wetting by water droplets. J. Phys. Chem. B 109, 15454–15462 (2005).
Sakai, N., Fujishima, A., Watanabe, T. & Hashimoto, K. Enhancement of the photoinduced hydrophilic conversion rate of TiO2 film electrode surfaces by anodic polarization. J. Phys. Chem. B 105, 3023–3026 (2001).
Monteleone, F. V. et al. Light-controlled directional liquid drop movement on TiO2 nanorods-based nanocomposite photopatterns. Langmuir 26, 18557–18563 (2010).
Baigl, D. Photo-actuation of liquids for light-driven microfluidics: state of the art and perspectives. Lab Chip. 12, 3637–3653 (2012).
Hashimoto, K., Irie, H. & Fujishima, A. TiO2 photocatalysis: a historical overview and future prospects. Jpn J. Appl. Phys. 1 44, 8269–8285 (2005).
Irie, H., Washizuka, S., Yoshino, N. & Hashimoto, K. Visible-light induced hydrophilicity on nitrogen-substituted titanium dioxide films. Chem. Commun. 39, 1298–1299 (2003).
Wang, R., Sakai, N., Fujishima, A., Watanabe, T. & Hashimoto, K. Studies of surface wettability conversion on TiO2 single-crystal surfaces. J. Phys. Chem. B 103, 2188–2194 (1999).
Sakai, N., Fujishima, A., Watanabe, T. & Hashimoto, K. Quantitative evaluation of the photoinduced hydrophilic conversion properties of TiO2 thin film surfaces by the reciprocal of contact angle. J. Phys. Chem. B 107, 1028–1035 (2003).
Oregan, B. & Gratzel, M. A low-cost, high-efficiency solar-cell based on dye-sensitized colloidal TiO2 films. Nature 353, 737–740 (1991).
Bach, U. et al. Solid-state dye-sensitized mesoporous TiO2 solar cells with high photon-to-electron conversion efficiencies. Nature 395, 583–585 (1998).
Gratzel, M. Photoelectrochemical cells. Nature 414, 338–344 (2001).
Hardin, B. E., Snaith, H. J. & McGehee, M. D. The renaissance of dye-sensitized solar cells. Nat. Photonics 6, 162–169 (2012).
Gratzel, M. Dye-sensitized solar cells. J. Photochem. Photobiol. C 4, 145–153 (2003).
Qin, Y. C. & Peng, Q. Ruthenium sensitizers and their applications in dye-sensitized solar cells. Int J Photoenergy 2012, 291579 (2012).
Grunze, M. Surface science-driven liquids. Science 283, 41–42 (1999).
Zhang, L. B., Zhong, Y. J., Cha, D. & Wang, P. A self-cleaning underwater superoleophobic mesh for oil-water separation. Sci. Rep. 3, 2326 (2013).
Gao, S. J., Shi, Z., Zhang, W. B., Zhang, F. & Lin, J. Photoinduced superwetting single-walled carbon nanotube/TiO2 ultrathin network films for ultrafast separation of oil-in-water emulsions. ACS Nano 8, 6344–6352 (2014).
Wayment-Steele, H. K. et al. Monitoring N3 dye adsorption and desorption on TiO2 surfaces: a combined QCM-D and XPS study. ACS Appl. Mater. Inter. 6, 9093–9099 (2014).
Mohsen Oftadeh, L. T. Investigation of optoelectronic properties of N3 dye-sensitized TiO2 nano-crystals by hybrid methods: ONIOM (QM/MM) calculations. Int. Nano Lett. 3, 26 (2013).
Fujishima, A., Zhang, X. T. & Tryk, D. A. TiO2 photocatalysis and related surface phenomena. Surf. Sci. Rep. 63, 515–582 (2008).
Kwon, G. et al. On-demand separation of oil-water mixtures. Adv. Mater. 24, 3666–3671 (2012).
Jen-Shih Chang, A. J. K. & Joseph, M. C. Handbook of Electrostatic Processes CRC Press (1995).
Pabby, A. K., Rizvi, S. S. H. & Sastre Requena, A. M. Handbook of Membrane Separations: Chemical, Pharmaceutical, Food, and Biotechnological Applications CRC Press (2008).
Kota, A. K., Kwon, G., Choi, W., Mabry, J. M. & Tuteja, A. Hygro-responsive membranes for effective oil-water separation. Nat. Commun. 3, 1025 (2012).
Mugele, F. Fundamental challenges in electrowetting: from equilibrium shapes to contact angle saturation and drop dynamics. Soft Matter 5, 3377–3384 (2009).
Mugele, F. & Baret, J. C. Electrowetting: from basics to applications. J. Phys. Condens. Mat. 17, R705–R774 (2005).
Pelet, S., Moser, J. E. & Gratzel, M. Cooperative effect of adsorbed cations and iodide on the interception of back electron transfer in the dye sensitization of nanocrystalline TiO2 . J. Phys. Chem. B 104, 1791–1795 (2000).
Clifford, J. N., Palomares, E., Nazeeruddin, M. K., Gratzel, M. & Durrant, J. R. Dye dependent regeneration dynamics in dye sensitized nanocrystalline solar cells: evidence for the formation of a ruthenium bipyridyl cation/iodide intermediate. J. Phys. Chem. C 111, 6561–6567 (2007).
Boschloo, G. & Hagfeldt, A. Characteristics of the iodide/triiodide redox mediator in dye-sensitized solar cells. Accounts Chem. Res. 42, 1819–1826 (2009).
Antila, L. J., Myllyperkio, P., Mustalahti, S., Lehtivuori, H. & Korppi-Tommola, J. Injection and ultrafast regeneration in dye-sensitized solar cells. J. Phys. Chem. C 118, 7772–7780 (2014).
Montanari, I., Nelson, J. & Durrant, J. R. Iodide electron transfer kinetics in dye-sensitized nanocrystalline TiO2 films. J. Phys. Chem. B 106, 12203–12210 (2002).
Bauer, C., Boschloo, G., Mukhtar, E. & Hagfeldt, A. Interfacial electron-transfer dynamics in Ru(tcterpy)(NCS)(3)-sensitized TiO2 nanocrystalline solar cells. J. Phys. Chem. B 106, 12693–12704 (2002).
Haque, S. A., Tachibana, Y., Klug, D. R. & Durrant, J. R. Charge recombination kinetics in dye-sensitized nanocrystalline titanium dioxide films under externally applied bias. J. Phys. Chem. B 102, 1745–1749 (1998).
Cahen, D., Hodes, G., Gratzel, M., Guillemoles, J. F. & Riess, I. Nature of photovoltaic action in dye-sensitized solar cells. J. Phys. Chem. B 104, 2053–2059 (2000).
Tian, D. L. et al. Patterned wettability transition by photoelectric cooperative and anisotropic wetting for liquid reprography. Adv. Mater. 21, 3744–3749 (2009).
Westerlund, S. & Ekstam, L. Capacitor theory. IEEE T. Dielect. El. In. 1, 826–839 (1994).
Haynes, W. M. CRC Handbook of Chemistry and Physics 96th edn CRC Press (2015).
Jeon, J., Goddard, W. A. & Kim, H. Inner-sphere electron-transfer single iodide mechanism for dye regeneration in dye-sensitized solar cells. J. Am. Chem. Soc. 135, 2431–2434 (2013).
Liu, Z. Y. et al. Solution-processed organic photovoltaics based on indoline dye molecules developed in dye-sensitized solar cells. Molecules 18, 3107–3117 (2013).
Wang, X. F. & Kitao, O. Natural chlorophyll-related porphyrins and chlorins for dye-sensitized solar cells. Molecules 17, 4484–4497 (2012).
Lightbourne, S. K. S., Gobeze, H. B., Subbaiyan, N. K. & D’Souza, F. Chlorin e6 sensitized photovoltaic cells: effect of co-adsorbents on cell performance, charge transfer resistance, and charge recombination dynamics. J. Photon. Energy 5, 053089 (2015).
Eow, J. S. & Ghadiri, M. Electrostatic enhancement of coalescence of water droplets in oil: a review of the technology. Chem. Eng. J. 85, 357–368 (2002).
We acknowledge financial support from the King Fahd University of Petroleum and Minerals (KFUPM) through the Center for Clean Water and Clean Energy at MIT and KFUPM (project no. R15-CW-11).
The authors declare no competing financial interests.
Supplementary Figures, Supplementary Tables, Supplementary Notes and Supplementary References (PDF 1624 kb)
This movie demonstrates the photo-induced anisotropic wetting of a NaCl droplet on a Chlorin dye-sensitized TiO2 surface. When focused white light shines on one edge of the droplet, the droplet spreads towards the illuminated edge while the other side is pinned. (MOV 1761 kb)
This movie demonstrates the demulsification of Span80-stabilized brine (10 wt% NaCl in water)-in-dodecane emulsion. The stainless steel mesh (pore size ≈ 2 μm) coated with Chlorin dye-sensitized TiO2 nanostructured film is sandwiched between the two vertical glass tubes. Brine droplets that contact the Chlorin dye-sensitized TiO2 mesh surface spread and coalesce with other droplets under white light illumination. Within minutes of illumination, the brine-in-dodecane emulsion demulsifies into brine-rich and dodecane-rich phases. (MOV 672 kb)
About this article
Cite this article
Kwon, G., Panchanathan, D., Mahmoudi, S. et al. Visible light guided manipulation of liquid wettability on photoresponsive surfaces. Nat Commun 8, 14968 (2017). https://doi.org/10.1038/ncomms14968
Moses Effect: Splitting a Sessile Droplet Using a Vapor-Mediated Marangoni Effect Leading to Designer Surface Patterns
ACS Applied Materials & Interfaces (2020)
Tunable Fluorescence and Room-Temperature Phosphorescence from Multiresponsive Pure Organic Copolymers
Industrial & Engineering Chemistry Research (2020)
Selective Wettability Membrane for Continuous Oil−Water Separation and In Situ Visible Light‐Driven Photocatalytic Purification of Water
Global Challenges (2020)