Yong Guan1, Chenchen Yu1, Jiawen Zhu1, Rui Yang1, Xiang Li1, Dafu Wei1, Xiang Xu1. 1. Key Laboratory for Ultrafine Materials of Ministry of Education, School of Materials Science and Engineering, East China University of Science and Technology Shanghai 200237 P. R. China dfwei@ecust.edu.cn xiangxu@ecust.edu.cn.
Superhydrophobic technologies derived from nature, typically like the “lotus effect”, have attracted much attention around the world both in academic research and in industry applications. Dirt particles on lotus leaves can be easily removed by water droplets due to the hierarchical structures of the surface, which are formed out of a characteristic epidermis and covering of waxes.[1] Similar non-wettable properties are also prevalent among animals, like water striders and flying insects.[2,3] Those surfaces show tremendous value in anticorrosion, self-cleaning, drag reduction, oil-water separation and other fields.[4-6] In general, the superhydrophobic property can be obtained using materials with low surface energy and by constructing morphological structures.[7,8]Many research works have been reported on artificial superhydrophobic surfaces by controlling the chemical composition of polymers[9] and metals[10,11] or by fabricating novel structures using various techniques such as phase separation,[12] polymer imprinting,[13] sol–gel processing,[14] chemical etching[15] and others.[16] However, these methods are usually complex and time-consuming. Therefore, it is crucial to develop a simple and effective approach to fabricate a superhydrophobic coating which is suitable for the manufacture in a large scale. Dip-coating is thought to be one of the most promising methods since it is low-cost and less demanding for production facilities. Furthermore, considering that the components applied in superhydrophobic surfaces like perfluoroalkylsilane are usually expensive and ecologically unfriendly,[17-20] it is more provident to develop a superhydrophobic surface using fluorine-free and sustainable materials.[21-24]Fabricating hierarchical structures in micro- and nanoscale is an important concept to create a superhydrophobic coating. Inorganic nanoparticles like SiO2 and TiO2, combined with organic polymers,[25] are usually used to improve the hydrophobicity and surface roughness of the coating. Nevertheless, those hierarchical structures are usually fragile which exhibited poor resistance to mechanical scratch and abrasion since nanoparticles are difficult to cooperate with the organic polymer materials.One effective solution is to acquire a strong bonding of inorganic nanoparticles to the matrix resin by adding a cross-linking agent,[26,27] endowing the coatings with superhydrophobicity and abrasion resistance. Another useful method is to apply an external process like thermal annealing, to form “welding” between polymer matrix and particle interfaces,[28,29] which could greatly enhance the durability of hierarchical structures.Inspired by the epicuticular wax on lotus surface, some efforts have been made to render wax with superhydrophobicity through the fabrication of hierarchical structures, among which a typical method is phase separation. Some researchers used a combination of solvent and nonsolvent to create phase separation of wax. Lu et al.[30] prepared a low-density polyethylene superhydrophobic surface by controlling its crystallization behavior in a xylene–cyclohexanone mixture. However, those solvents were usually toxic and harmful, thus limiting the application of coatings. Other researchers chose mixed wax for the phase separation during drying process. Zhang et al.[31] endowed paper surface with superior superhydrophobicity via the phase separation of green-based waxes. Wang et al.[32] used the beeswax and carnauba wax to fabricate nontoxic superhydrophobic coatings that could be applied on food containers. Though hierarchical bulbiform shapes in microscale could be generated in this way, the components were stacked on the surface randomly thus might be easily buried underneath, which would lead to structure defects.In this work, a vapor-induced method using fluorine-free materials to fabricate superhydrophobic surfaces was reported. Organic components (hydroxyl acrylic resin, cross-linking agent as well as PEW) and inorganic components (SiO2) were mixed in ethyl acetate to make a homogeneous suspension for dip-coating. The coating was endowed with a micro/nano-structure and enhanced roughness simultaneously through a simple control of preparation process, boosting the operation flexibility compared with the complicated methods reported previously. PEW could be dispersed evenly in ethyl acetate with other components due to its low melting point, therefore eliminating the usage of toxic organic solvent. By the virtue of the high reactivity of isocyanate groups with silanol and hydroxyl groups, hydroxyl acrylic resin and SiO2 were cured by the cross-linking agent as a basic hydrophobic rough layer onto the surface of glass slides. Therefore, a rather reinforced coating was formed, partly offsetting the mechanical weakness of hydrophobic coatings. Moreover, PEW emulsions were crystallized into uniform whiskers under the induction of ethyl acetate vapor, and a carpet-like surface was formed with the increase of PEW content, which greatly increased the surface roughness and endowed the coating with superhydrophobicity and antifouling ability. Additionally, different preparation conditions were compared to explore their effects on surface morphology and superhydrophobicity. The coatings were characterized by scanning electron microscope, FT-IR and contact angle/interface system. Self-cleaning test and mechanical durability test were used to evaluate the performance of the composite coating.
Experimental
Materials
Polyethylene wax (PEW-G500) was supplied by Kaikai Technology & Trade Co., Ltd. (China). Hydroxyl acrylic resin (AMS 2788) was purchased from Guangzhou Yuemei Chemical Co., Ltd. (China). Silica nanoparticles (SiO2-R812) with an average particle size (7–40 nm) was provided by Evonik Industries AG (Germany). Hexamethylene diisocyanate trimer (HDI trimer-N3390) acting as a cross-linking agent was bought from Bayer (Germany), and ethyl acetate in analytical purity was provided by Shanghai Titan Scientific Co., Ltd. (China). All chemicals were used without further purification.
Preparation of SPEW coatings
3 g of SiO2, and 1.2 g of hydroxyl acrylic resin were ultrasonically dispersed in 100 ml ethyl acetate for 30 min to form a homogeneous suspension. A series amount of PEW (10 wt% to 25 wt%) were added into the suspension and the mixture was magnetically stirred in a water bath at 70 °C for 30 min, then 0.4 g of HDI trimer was added into the suspension followed by another 5 min stirring. After that, the mixture was cooled to 30 °C at room temperature, and the hybrid coating was fabricated by a simple dip-coating method using glass slides, which were washed with ethyl acetate successively for several times. Then the coated slides were put in the oven at 80 °C for 2 min, and finally cured at room temperature for 24 h to obtain a silica-PEW (SPEW) composite coating.
Characterization of SPEW coatings
Surface morphology
The surface morphology was observed by a scanning electron microscope (SEM, S-3400N, Hitachi) with an acceleration voltage of 15 kV after gold-sputtering for 1 min. Coverslips were used to prepare SPEW coating samples for gold-sputtering.
Structure
The spectra of samples were recorded on a FT-IR analyzer (Nicolet 6700, Thermo Electron) from 4000 to 500 cm−1. SiO2 and hydroxyl acrylic resin were ground with KBr respectively to form a pellet to record the FT-IR spectra. The reaction products of SiO2 and hydroxyl acrylic resin with HDI trimer were reserved on a coverslip and recorded in a reflection mode. HDI trimer was coated on a KBr crystal window to obtain the FT-IR spectra in a coating method.
Contact angle and sliding angle
Contact angle and sliding angle measurements were performed using a contact angle/interface system (JC2000D3, Shanghai Zhongchen Digital Technical Apparatus) at room temperature. A 5–8 μl of water droplet was placed onto the samples and the final value was obtained from the average of 5 measurements in different locations for each sample.
Self-cleaning test
Various food liquids including ketchup, orange juice, cola, vinegar and yogurt were used for the repelling test. The liquid droplets were dropped from top of coated slides, which were put in a certain gradient to observe the repelling performance along the rolling paths. For dirt-removal test, 3 g of dusts in diameter of ca. 500 μm were put onto the samples to create an artificially contaminated surface. Then the samples were immersed in cyclohexane or hexadecane, and water dyed by ink were dropped onto the coated surface to test the self-cleaning property.
Mechanical durability test
Knife-scratch, sandpaper abrasion and tape peeling tests were carried out to test the mechanical durability of the SPEW coating. For knife-scratch test, sparse and intensive cross-scratches were applied respectively on the surfaces to evaluate the scratch resistance property. For the sandpaper abrasion resistance test, the coated glass slide (25 mm × 75 mm) under 100 g of loading was placed face-down to the 2000 mesh sandpaper. The surface was moved back and forth along the ruler from one side to another parallel to the sandpaper. 10 cm of the moving distance was recorded as one cycle of the abrasion test. In the tape peeling test, an adhesive tape (Scotch-600 tape) was glued to the sample surface and tightly pressed, then was removed by peeling. The resulting surface was observed with SEM. Water was dropped on different points to measure the contact angles after knife-scratch, sandpaper abrasion and tape peeling tests.
Results and discussion
Molecular structures of nanoscale coatings
The FTIR spectra of the components SiO2, hydroxyl acrylic resin, HDI trimer as well as the reaction products are shown in Fig. 1. Based on the relative absorbance intensity of functional groups, it was discovered that hydroxyl groups of acrylic resin 3480 cm−1 and silanol groups of SiO2 at 3414 cm−1 almost disappeared due to the possible reaction with isocyanate groups in HDI trimer, while C–H group at 2935 cm−1 in the acrylic resin and Si–O–Si groups at 1086 cm−1 in SiO2 still remained. In the FTIR spectrum of HDI trimer, two intense peaks at 1688 cm−1 and 2277 cm−1 were assigned to stretching vibrations of CO bond and –NCO groups, respectively. However, the absorbance intensity ratio of –NCO groups to CO bond dramatically decreased in reaction products compared with that of HDI trimer, which indicated that most of the –NCO groups were consumed during the curing process and transferred into a –O–C(O)–NH– structure. Based on the above analysis, the possible chemical bondings among SiO2, hydroxyl acrylic resin, HDI trimer and glass slides are displayed Scheme 1. The newly formed –O–C(O)–NH between glass slides and HDI trimer helped to form a stable and robust composite coating.
Fig. 1
FTIR spectra of HDI trimer, hydroxyl acrylic resin, SiO2 and reaction products.
Scheme 1
Possible bonding structures among SiO2, hydroxyl acrylic resin and HDI trimer on glass slides.
Micro-morphology of superhydrophobic SPEW composite coatings
The SEM images as well as the images of water contact angles of surface of SPEW coatings with varied PEW weight ratio are shown in Fig. 2. The particular PEW microscale structures were observed with the addition of PEW. When 10 wt% of PEW was added into the mixture, a small amount of PEW whiskers randomly dispersed on the coating surface, displaying a contact angle of 131° ± 2° (Fig. 2a). With the increase of PEW content from 15 wt% to 20 wt%, more PEW clusters formed and the surfaces became much rougher (Fig. 2b), showing contact angles rising from 147° ± 3° to 153° ± 1°. The hydrophobic coating was successfully transferred into a superhydrophobic coating. As the PEW content was continuously increased to 25 wt%, a homogeneous micro- and nanoscale hierarchical structure was fabricated (Fig. 2d), and the contact angle further increased to 163° ± 5°. In the SEM expansion images of coatings (Fig. 2a), the PEW whiskers in Fig. 2d was observed to provide a more efficient air gap compared with those of other coatings, and acted as a full-scale protection to prevent the coating from being contaminated.
Fig. 2
SEM images of micro–nanoscale structures of SPEW coatings with various PEW dosages. (a1) 10 wt%, (b1) 15 wt%, (c1) 20 wt%, (d1) 25 wt%; (a2–d2) expansion images from (a1–d1).
Formation mechanism of superhydrophobic surface
The formation mechanism of surface morphology is illustrated in Scheme 2. The mixture was stirred at 70 °C until a uniform suspension was formed. The inorganic hydrophobic nanoparticles were easily suspended in the PEW emulsion due to similar polarities. In the followed cooling process until 30 °C, PEW crystal nucleuses in microscale were gradually deposited out of the mixture. Then glass slides were fastly dip-coated and put immediately in an oven at 80 °C for 2 min. As the solvent evaporated during the drying process, SiO2 particles slowly precipitated onto the interface between mixture and slide due to a higher density, and formed a loose hydrophobic layer. Meanwhile, the solvent underneath was evaporated in a slower rate through the voids among nanoparticles. It is worth mentioning that by the virtue of a lower density, PEW crystal nucleuses gradually migrated to the upper layer during the evaporation of solvent. Since the drying temperature was 10–20 °C higher than the melting point of PEW, crystal nucleuses were transferred into a near molten state, and then slowly shaped to small whiskers induced by ethyl acetate vapor. The samples were then slowly cured at room temperature for 24 h, which provided a condition for the growth of PEW whiskers. Finally, a micro–nanoscale composite coating with relatively high surface roughness was fabricated.
Scheme 2
Schematic illustration for the formation of superhydrophobic surface.
In order to further investigate the influence of preparation conditions on surface morphologies, different coatings with 25 wt% of PEW were prepared, as the results are shown in Table 1 and Fig. 3. Sample E was the same as sample d in Fig. 2. Compared with sample C, D and E to cool to 30 °C, it took more time for sample A to cool to 25 °C, which resulted in lager crystal nucleuses of PEW. These crystals might be difficult to be transferred into a near molten state at 80 °C in 2 min, affecting the re-shaped process induced by ethyl acetate vapor, thus depositing in a random shape with a diameter of 1–3 μm on the surface, as shown in Fig. 3a.
Process parameters of different coatings
Samples
Process
Cooling
Drying
Contact angles
A
Cooling/drying
To 25 °C, no stirring
80 °C, 2 min
132° ± 2°
B
Drying
—
80 °C, 2 min
141° ± 1°
C
Cooling/drying
To 30 °C, stirring
80 °C, 2 min
130° ± 3°
D
Cooling/drying
To 30 °C, no stirring
80 °C, 5 min
135° ± 2°
E
Cooling/drying
To 30 °C, no stirring
80 °C, 2 min
163° ± 5°
Fig. 3
SEM images of coatings prepared in different conditions. (a) Cooled to 25 °C, (b) without cooling process, (c) cooling with stirring, (d) dried at 80 °C for 5 min.
In contrast with sample A, many small PEW whiskers in a diameter of 100–300 nm formed on the surface of sample C (Fig. 3c). It might be owed to the shearing effect from stirring during the cooling process, which prompted the formation of many small crystal nucleuses. It was noticed that the coating of sample B, which was dried directly without cooling process, was netlike and consisted of entangled pores with a diameter in the range of several micrometers (Fig. 3b). It confirmed that PEW suspension under a molten state was thermodynamically unstable when evaporating the solvent. As a result, phase separation would occur to form a PEW rich phase and a PEW poor phase. The rich phase solidified and formed the matrix after drying the solvent, whereas the PEW poor phase formed the pores. In addition, the hierarchical structures fabricated by present method remarkably increased the surface roughness, displaying an increased water contact angle to 141° ± 1°. Since the drying temperature was much higher than the melting point of PEW, a similar effect on the surface morphologies was observed by raising the drying temperature or prolonging the drying time. Sample D was dried for a longer time compared with other coatings. As a result, PEW crystals were remelted into liquid drops during the evaporation of solvent. However, those drops wrapped with nanoparticles could not aggregate together and then were stacked randomly on the surface, as shown in Fig. 3d. Therefore, the detailed surface morphologies could be controlled by changing the cooling and drying conditions during the process, which was also reported by other researches, such as netlike hollow structures resulting from phase separation.[33] Nevertheless, the carpet-like morphology was seldom illustrated, and its performance was rarely investigated.
Applications of SPEW coatings
The coating of 25 wt% PEW content was chosen to investigate its applications due to its more compact micro structures and superior superhydrophobicity. Various substrates were used for the characterization of superhydrophobicity, including filter paper, cotton, textile, glass slides and tinplate, as shown in Fig. 4. Dyed water droplets were placed on the white coated surfaces and the uncoated surfaces, respectively. The composite coating on various substrates exhibited an outstanding super-repellency property to water droplets, which still maintained their sphere-like shapes on different points of coated surfaces. For some substrates with certain inherent interspace, such as cotton and textile (Fig. 4a and c), water droplets easily penetrated through those uncoated surfaces. However, on all the coated surface droplets maintained their sphere-like shapes and easily rolled off from the surfaces, indicating a perfect adaptability of the composite coating on both hard (glass and tinplate) and soft (filter, paper, cotton and textile) substrates. It should be noted that the coated surfaces were white and non-transparent, which may partly limit their practical applications.
Fig. 4
Dyed water droplets on the coated and uncoated surfaces of cotton (a), filter paper (b), textile (c), glass slide (d) and tinplate (e).
Self-cleaning property of SPEW coatings
In order to further evaluate the performance of composite coating, various liquids were used for the repelling test, such as some food liquids in the reported work.[34]Fig. 5 showed the pictures of these liquids on the composite coating, as well as the corresponding contact angles and sliding angles. Ketchup, orange juice, cola, vinegar and yogurt maintained the spherical shapes with high contact angles and low sliding angles while olive oil and cooking oil spread out on the surface, showing a lipophilic property of the coating. Since PEW and hydrophobic SiO2 are both lipophilic, it's reasonable that the coating could not repel oil. And further addition of materials with low surface energy could be one of the potential methods to vest the coating with oleophobic property.[35,36]
Fig. 5
Various liquid repelling tests on the coated surfaces (left) and their contact angles/sliding angles (right).
Rolling processes of various liquids are shown in Fig. 6, with contact angle images placed on the bottom right corner. Coated surfaces were put in a certain slope before test. For ketchup and yogurt tests, the coated slides were put in a higher slope (45° and 30°) for a smoother rolling process. When those liquids were dropped on the coating, they could completely roll off from the surfaces with no residual trace. Therefore, the coating could maintain its surface cleanness against both light liquids and thick liquids.
Fig. 6
Rolling processes of ketchup (a1–a3), orange juice (b1–b3), cola (c1–c3), vinegar (d1–d3), yogurt (e1–e3) on the coated surfaces.
Self-cleaning tests under hydrophobic solvent system was rarely reported probably due to the loss of water repellency when superhydrophobic surfaces are contaminated by hydrophobic solvent.[37] In this work, the uncoated and coated glass slides with dust contamination were immersed in cyclohexane and the processes of removing the dust were recorded when water droplets rolled over the dust to further evaluate the self-cleaning property of the coating, as presented graphically in Fig. 7. Fig. 7a showed that when water droplets rolled off from glass slides, they spread in a random shape, and the dust still remained along the path. In contrast, the composite superhydrophobic coating allowed water droplets to take the dust away from its rolling and bouncing path, as shown in Fig. 7b, indicating that the self-cleaning property was still retained even after cyclohexane-contamination. Changing cyclohexane to hexadecane, the same results of dust successfully removed on the coating surface were observed, further indicating an excellent self-cleaning property of the SPEW coating.
Fig. 7
Self-cleaning test on uncoated surface (a1–a3) and coated surface (b1–b3) when surfaces immersed in cyclohexane.
Durability of SPEW coatings
Durability of superhydrophobic coatings is a crucial factor that limits their widespread applications, since micro- and nanostructures may be destroyed when faced with mechanical friction, leading to the loss of superhydrophobicity. Here, knife-scratch, sandpaper abrasion and tape peeling tests were used to evaluate the mechanical durability of the SPEW coating. As shown in Fig. 8a, sparse (A) and intensive (B) cross-scratches were applied respectively on the coated surfaces to imitate the scratch conditions in practical applications, and water droplets were placed on the surfaces after knife-scratch (Fig. 8b). It was noticed that the coating still retained their non-wetting property, regardless of sparse or intensive cross-scratches. The contact angles were 158° ± 2° (A) and 153° ± 2° (B) respectively, indicating that scratching did not induce a significant decrease of the superhydrophobicity on the SPEW coating.
Fig. 8
Knife-scratch test. Sparse and intensive cross-scratches on the coated surfaces (a), water droplets on the scratched surfaces (b).
In sandpaper abrasion test, water contact angles and sliding angles were recorded after a certain number of abrasion cycles, shown in Fig. 9, and SEM images before and after 25, 40 abrasion cycles are shown in Fig. 10. When the PEW whiskers that protruded onto the SPEW surface (Fig. 10a) were first removed, the contact angles decreased a little from 163° ± 5° to 159° ± 1°. As the number of abrasion cycles increased, part of PEW micro structures was destroyed, resulting in the decrease of contact angles and increase of sliding angles. However, the coating still kept its superhydrophobicity after 25 cycles of abrasion, with a contact angle of 152° ± 3° and sliding angle of 9° ± 2°. Fig. 10b showed that some PEW whiskers still remained and SiO2 nanoparticles stacked on the whiskers, which helped to maintain the superhydrophobicity of coating. However, a significant decrease of contact angle was noticed after 30 cycles of abrasion, leading to the loss of superhydrophobicity. It might owe to the destruction of PEW whiskers microscale structures after multiple abrasion cycles, leaving the nanoscale structures consisting of SiO2 to resist the abrasion from sandpaper, as SEM image shown in Fig. 10c. In the test after 30 cycles, the contact angles and sliding angles had no remarkable change, showing the increasing durability of nanoscale layer, which might relate with the firm bonding of SiO2 with hydroxyl acrylic resin due to the reaction among SiO2, hydroxyl acrylic resin and HDI trimer.
Fig. 9
Water contact angles and sliding angles of SPEW coating during 40 abrasion cycles.
Fig. 10
SEM images of coatings before (a) and after 25 abrasion cycles (b), 40 abrasion cycles (c).
EDX spectra of the coatings before and after 25, 40 abrasion cycles were also recorded to study the changes of surface element content, shown in Fig. 11. For the surface almost covered with PEW whiskers before abrasion, the atomic signal of Si was relatively weak. Compared with the benchmark peak at 0 keV, the samples after 25 and 40 abrasion cycles showed much higher Si content on their surfaces, due to a raising number of bare SiO2 nanoparticles during the process of abrasion test.
Fig. 11
EDX spectra of coatings before (a) and after 25 abrasion cycles (b), 40 abrasion cycles (c).
To further test the tolerance to common damages, the superhydrophobic coating was then treated with tape peeling, shown in Fig. 12. It could be clearly observed that the PEW whiskers on the surface were removed by tape peeling but the nanoscale layer resisted the external force and remained. Under the combined effect of SiO2, hydroxyl acrylic resin and cross-linking agent, the coating could still maintain a favourable hydrophobicity, with a water contact angle of 140° ± 3° on its surface.
Fig. 12
SEM images of coatings before (a) and after (b) tape peeling.
Conclusions
A self-cleaning and mechanically durable superhydrophobic coatings with hierarchical structures were successfully constructed by a simple vapor-induced method. The immersion suspension composed of ethyl acetate, silica nanoparticles (SiO2), hydroxyl acrylic resin, cross-linking agent and polyethylene wax (PEW). Various substrates were dip-coated in the suspension, subsequently controllably dried, forming hierarchical structure surfaces with PEW whiskers outer layer in microscale and SiO2 inner layer in nanoscale. The introduced hydroxyl acrylic resin with remarkable wear resistance and adhesion property effectively connected with SiO2 nanoparticles, ensuring the hydrophobicity and durability of inner layer. Moreover, at a suitable protocol of the dip-coating at 30 °C and drying at 80 °C for 2 min as well as 25 wt% of PEW, uniform PEW whiskers formed in carpet-like shapes and the coating transferred into a superhydrophobic coating with a water contact angle of 163° ± 5°, excellent self-cleaning property even under solvent-contamination. Besides, the superhydrophobic coating could bear fairly intensive knife-scratch, tape peeling and 25 cycles of sandpaper abrasion under 100 g of loading.
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