Journal of Nanomaterials

Journal of Nanomaterials / 2017 / Article

Research Article | Open Access

Volume 2017 |Article ID 2102467 |

Veromee Kalpana Wimalasiri, Helapiyumi Uthpala Weerathunga, Nilwala Kottegoda, Veranja Karunaratne, "Silica Based Superhydrophobic Nanocoatings for Natural Rubber Surfaces", Journal of Nanomaterials, vol. 2017, Article ID 2102467, 14 pages, 2017.

Silica Based Superhydrophobic Nanocoatings for Natural Rubber Surfaces

Academic Editor: Silvia Licoccia
Received30 Mar 2017
Revised01 Jun 2017
Accepted19 Jun 2017
Published08 Aug 2017


Silica based nonfluorinated superhydrophobic coatings for natural rubber surfaces have been developed. The coating was synthesized using nanosilica dispersion and a polychloroprene type binder as a compatibilizer. This nanocoating of silica was applied on to the surface of finished natural rubber gloves, by spray coating or dipped coating methods. The nanocoating demonstrates a water contact angle of more than 150° and sliding angle of 7°. The morphological features of the coating have been studied using scanning electron microscopy and atomic force microscopy while Fourier transform infrared spectroscopy was used to understand the nature of surface functional groups. Both imaging techniques provided evidence for the presence of nanosized particles in the coating. Coated gloves demonstrated comparable mechanical properties and significantly better alcohol resistivity when compared to those of the uncoated gloves.

1. Introduction

Nanotechnology has recently gained the industrial attention as a sustainable way to solve many of the problems associated with the current society. It has been effectively implemented in many fields such as agriculture, water purification, energy, and medical and polymer industry [1]. Amongst these applications many functional nanomaterials have been utilized in polymer industry in order to impart various properties to the products.

The concept of superhydrophobicity has been widely exploited during the past decade due to the potential applications in impermeable textiles, self-cleaning coatings, lab-on-a-chip devices, microfluidic devices, and glasses [27]. A surface is defined as superhydrophobic when its contact angle is more than 150° and the sliding angle is less than 10° [8]. This phenomenon is naturally observed in numerous biological surfaces such as the lotus leaf, the namib, the desert beetle, and the water strider [911]. Thus, many methods in creating superhydrophobicity on different material surfaces have been achieved through the biomimetic approach [12, 13].

Yu et al. have synthesized hydrophobic silica aerogel spheres by a coprecursor method. Here, a contact angle of 152° was achieved [14]. Seyedmehdi et al. have also synthesized superhydrophobic room temperature vulcanized silicone rubber insulator coatings with a contact angle of 145° and good UV durability [15]. Meanwhile, nanoscale surface roughness has been achieved by Mates et al. using paraffin wax-polyolefin thermoplastic blend (elastomer matrix binder) with bulk-produced carbon nanofibers as a stretchable coating for low-cost ultraflexible electronics [16]. Moreover, superhydrophobicity has been obtained by Bayer et al. using different types of rubber reinforced biopolymer/organoclay nanocomposite coatings. Here, a biolubricant has been used to cause hydrophobic phase inversion. Synthetic and fluoroacrylic rubber containing nanocomposite have shown better self-cleaning properties than natural rubber reinforced nanocomposite [17].

Silicone rubber and nanofluoric particles have been mixed in order to obtain superhydrophobic characteristics on silicon rubber surfaces by Seyedmehdi et al. [18]. Kato et al. have reported the synthesis of silica-filled cross-linked natural rubber which exhibit both hydrophobic and hydrophilic properties [19]. Simpson et al. have reviewed historic limitations of superhydrophobic surfaces and coatings, supplementing recent superhydrophobic breakthroughs such as resin marbles, volumetric superhydrophobic coatings, and water marbles which can be used for a wide range of applications [20]. Moreover, superhydrophobic aluminum surfaces have been fabricated using a simple spray coating approach where the coating consists of wear abrasion resistant acrylonitrile butadiene styrene rubber and hydrophobic silica nanoparticles. This superhydrophobic coating has shown extreme thermal properties which does not degrade until 420°C [21]. Historically, fluorinated hydrocarbon based coatings have been utilized in superhydrophobic applications. Silica sol-gel based coatings fabricated using long-chain fluoroalkylsilane was reported by Liu et al. recently, exhibiting a water contact angle of 169° [22]. However, these compounds are currently identified as carcinogenic where Wang et al. have reported polyfluorinated iodine alkanes can act on estrogen receptors subsequently, causing detrimental effects on reproductive and development systems [23]. Therefore, there is an increased interest in developing alternative coatings [24]. In this context, silica aerogels and silica based nanomaterials have been identified as potential materials.

Silica aerogels are translucent and thermal insulating materials consisting of nanosized pores, networked together to form an open, highly porous structure. As a result, they possess a large surface area (500–1500 m2/g), high porosity (80–99%), and low bulk density (0.03–0.35 g/cm3). In addition, they demonstrate small pore sizes ranging between 1 and 100 nm. Low index of refraction (~1.05) and high optical transmission (~93%) impart transparent characteristics into silica aerogel materials [2529]. In superhydrophobic applications, silica aerogel is generally modified with a suitable long-chain alkyl groups.

This study focuses on the development of a novel superhydrophobic nanocoating on natural rubber surfaces. An organically modified silica aerogel based coating formulation was developed where an added polychloroprene based polymer compatibalizes the coating onto the rubber surface. The structural features, mechanical properties, and chemical resistivity have been studied and compared with those of uncoated natural rubber gloves.

2. Experimental Methods and Materials

2.1. Materials

L-Turpentine (99%), ethyl acetate (≥99.5%), methanol (80%), and formic acid (>99%) were purchased from Sigma-Aldrich. Enova IC3100 silica aerogel (particle size 2–40 μm) was purchased from Cabot Cooperation. Deuterium oxide (99.9% atom D) was purchased from Sigma-Aldrich. Silicone sealant (BS 200 GP) was purchased from Bossil. Polymeric binder (refer to supplementary data, in Supplementary Material available online at (86%) was purchased from Sinwa Holdings, Sri Lanka. The molecules of all the ingredient materials are shown in Figure 1. Finished natural rubber gloves were purchased from a commercial supplier in Sri Lanka.

2.2. Experimental Procedure
2.2.1. Preparation of Silica Based Nanocoatings

The superhydrophobic coating solution was prepared by mixing 250 g of silicone sealant and 40 g of organically modified silica aerogel with 2 dm3 of turpentine. The mixture was stirred for one hour at 500 rpm and, then, it was sonicated for 10 minutes in an ultrasonic bath. The viscosity of the silica coating was optimized at a value of 1.2 Pa·s. The nanocoating was applied onto the natural rubber glove surface by dipped coating and spray coating methods.

2.2.2. Preparation of Compatibilizer Solution

The nanocoating and the rubber surface were compatibilized using an appropriate binder. The binder solution was prepared by mixing polychloroprene binder (500 g) with ethyl acetate (500 g) at a mixing ratio of 1 : 1 (w/w). The resulting mixture was stirred for one hour at 500 rpm at room temperature followed by ultrasound sonication for 10 minutes in an ultrasonic bath. After several trials the viscosity of the binder solution was optimized at a value of 1.4 Pa·s.

2.2.3. Application of Silica Nanocoating on to Natural Rubber Gloves: Dipped Coating Method

Vulcanized natural rubber gloves were dressed onto a ceramic former and dipped in the binder solution for 10 s after which the former was withdrawn. Then, the former was rotated in all 3 directions for about 40 s. The glove coated with the binder solution was then immersed (30 cm dipped length) in the silica dispersion for 10 s. The gloves were withdrawn from the silica dispersion in a slow manner (15 s withdrawal time per 30 cm length). The procedure was repeated to obtain two coatings and, then, the gloves were cured in an oven at 50°C for 24 h. The same procedure was repeated to coat a rubber film where the nanocoating did not contain silica aerogel. Figure 2 shows the appearance of a water drop upon contact with the coated and uncoated films.

2.2.4. Application of Silica Based Nanocoating onto Natural Rubber Gloves: Spray Coating Method

Natural rubber gloves were dressed onto a ceramic former and dipped in the binder solution for 10 s after which the former was withdrawn. Then, the former was rotated in all 3 directions for about 40 s. Subsequently, the silica dispersion was spray coated (H2000 mini HVLP traditional autospray gun with 0.8 mm nozzle supplied with 2 MPa compressed air). The distance between the nozzle of the gun and rubber surface was maintained at 10 cm. Silica dispersion (10 ml) was coated onto the glove surface. The former was rotated in all 3 directions for 1 min. This procedure was repeated to obtain two coatings. Then, the former was cured at 50°C for 24 h in an oven. The same procedure was repeated to coat a rubber film where the nanocoating did not contain silica aerogel. However this film did not show any superhydrophobic property.

2.3. Characterization
2.3.1. Stress-Strain Properties of the Coated Glove Samples

Both spray coated and dipped coated natural rubber gloves were tested for their stress and strain properties using Instron 55R1123 tensile testing machine. The coated rubber glove samples were molded into a dumbbell shaped test specimen (ASTM D412) using a mold. The length, width, and thickness of the samples were 70 mm, 10 mm, and 2.15 mm, respectively. The machine was equipped with a 1 kN load cell and operated at a crosshead speed of 500 mm/min.

2.3.2. Fourier Transform Infrared (FT-IR) Spectroscopy

The FT-IR spectrum of natural rubber, polychloroprene binder, and dipped coated and spray coated natural rubber materials were obtained using the diffuse reflectance mode over the range of 600–3500 cm−1 using Bruker Vertex 80 at a resolution of 4 cm−1.

2.3.3. Scanning Electron Microscope (SEM) Spectroscopy

Surface morphology characteristics of the superhydrophobic natural rubber materials were analyzed using a SU 6600 HITACHI scanning electron microscope (SEM) under the operating voltage of 5.0–10.0 kV. The glove samples were mounted onto an aluminum stub and a thin coating of gold was applied. The surface was imaged in the secondary electron mode. Quantitative analysis of the nanocoating was carried out using energy dispersing X-ray (EDX) analysis.

A drop of the liquid superhydrophobic nanocoating was kept over an aluminum SEM stub and was kept in the oven for 24 hours at 60°C for drying. After the drying process, a thin gold coating was applied. EDX analysis was replicated three times from three different places of the same specimen. The average values of the three readings were recorded.

2.3.4. Atomic Force Microscope (AFM) Spectroscopy

Three-dimensional surface features of the coated rubber material were observed and analyzed using a Park System AFM XE-100 microscope, under air at room temperature with a scanning rate of 0.5 Hz in noncontact mode with a 1650-00 type silicone tip.

2.3.5. Water Contact Angle (WCA) and Sliding Angle (SA) Measurements

A goniometer was used to measure the water contact angle of coated and uncoated rubber films. A high resolution digital camera (Cannon, macro mode) was used to capture the images which were set to the goniometer apparatus. Water droplet size used to measure contact angle was ~5 μL, and the droplet diameter was ~1 mm when it settled on the rubber surface. Five replicates were used to calculate an average contact angle value for each sample.

The same experiment was carried out for low molecular weight organic solvents and coconut oil to study the oleophobicity of the surface.

The sliding angle was measured with a sliding angle measurement system where the water droplet volume used for the measurement was 5 μL. Water droplet was kept on flat surface of the system. The sliding angles (the critical angle where a water droplet with a certain weight begins to slide down the inclined plate) were measured. Ten replicates were used to calculate an average sliding angle value for each sample.

2.3.6. Durability of the Nanocoating

An abrasion force was applied on the film using a disc shaped rough surface (25 kN). After each abrasion cycle contact angle of the surface was measured.

2.3.7. Permeability of Organic Solvents and Organic Acids

A special apparatus was designed (Figure 3) to study the permeability characteristics of the coated gloves towards organic solvents and dilute organic acids. A horizontal flow of the solvent and acid was maintained via the rubber film. The coated side of the rubber glove film was exposed to formic acid (6 cm3, 0.8 mol dm−3). The uncoated side of the rubber film was exposed to deuterium oxide (10 cm3 of D2O) as shown in Figure 3. The procedure was repeated for methanol (6 cm3, 0.8 mol dm−3) in order to understand the permeation properties of the film towards low molecular weight organic solvents. A Bruker Ascend TM 400 NMR spectrometer was used to detect the presence of formic acid/methanol in D2O. The time taken for solvent/acid to penetrate through the film was measured. The same procedure was repeated for the uncoated gloves as well. The morphological changes after the exposure to organic solvents/acid were studied using the SEM technique.

3. Results and Discussion

3.1. Mechanical Properties

Tensile and tear properties of the superhydrophobic gloves prepared by the spray and the dipped coating methods were compared with those of uncoated gloves (Table 1). The properties of spray coated gloves were similar to that of uncoated gloves while significant deterioration of mechanical properties was observed when the gloves were coated by the dipping technique. Unlike with the spray coating method, during the dipped coating, the rubber matrix is exposed to organic solvents for prolonged time intervals, leading to swelling of the natural rubber matrix. Such interactions lead to a reduction of mechanical properties and chemical changes in the structure of the polymer matrix can have a direct impact on the extent of interactions between the coating and the rubber glove.

ControlDipped coatedSpray coated

Cure time (hours)242424
Cure temperature (°C)505050
Tensile strength (MPa)16.22 ± 6.0911.58 ± 2.2415.65 ± 1.35
Mod 100% (MPa)1.40 ± 0.131.36 ± 0.081.44 ± 0.25
Mod 500% (MPa)8.35 ± 1.547.43 ± 2.448.58 ± 1.55
Tear strength (kN/m)43.48 ± 5.6629.39 ± 1.9030.52 ± 2.38

3.2. FT-IR Characterization of Natural Rubber and Coated Rubber

The FT-IR characterization data is summarized in Table 2 and shown in Figures 4 and 5. In the uncoated rubber film, intense peaks appearing between 3000 cm−1 and 2750 cm−1 are corresponding to CH2 symmetric stretching vibrations. In the coatings made by both spray and dipped coating methods, the above peaks appear at the same position, though with a significant reduction in their intensity. This concludes that the CH2 groups in natural rubber were unaffected by the interactions between the coating and natural rubber surface. The C=C of uncoated rubber was observed at 1660 cm−1. In the coated gloves this peak appears at 1657 cm−1, suggesting that the nanocoating had not chemically interacted with the double bonds of 1,4-polyisoprene units of the natural rubber.

Uncoated rubberCorresponding vibrationDipped coated rubberCorresponding vibrationSpray coated rubberCorresponding vibration
IR frequency (cm−1)IR Frequency (cm−1)IR Frequency (cm−1)

672C-H deformation686C-H deformation686C-H deformation
736C-H out of plane bending788Si-O symmetric stretching788Si-O symmetric stretching
836=C-H out of plane bending864=C-H out of plane bending864=C-H out of plane bending
1038C-H in plane bending1010C-H in plane bending1009C-H in plane bending
1091C-H in plane bending1072O-Si-O asymmetric stretching1072O-Si-O asymmetric stretching
1261O-P-O asymmetric1258O-P-O asymmetric stretching1258O-P-O asymmetric stretching
stretching1446CH2 deformation1446CH2 deformation
1375CH2 deformation1483CH2 deformation1483CH2 deformation
1445CH2 deformation1657C=C stretching1657C=C stretching
1660C=C stretching2853CH2 symmetric stretching2857CH2 symmetric stretching
2852CH2 symmetric stretching2921CH2 symmetric stretching2927CH2 symmetric stretching
2925CH2 symmetric stretching2962CH3 asymmetric stretching2962CH3 asymmetric stretching
2960CH3 asymmetric stretchingBroad peak in ~3500O-H stretchingBroad peak in ~3500O-H stretching
Broad peak in ~3500O-H stretching

The -CH2 deformation peaks appearing at 1375 cm−1 and 1445 cm−1 for natural rubber had shifted to 1446 cm−1 and 1483 cm−1, respectively, in the coated films. This significant change suggests that the free deformations of -CH2 are being affected by the presence of coating. Furthermore, C-H in plane bending peaks observed in uncoated samples appearing at 1038 cm−1 and 1091 cm−1 had shifted to 1009 cm−1 and 1010 cm−1, respectively, after coating [30, 31].

In pure silica aerogel, Si-O-Si asymmetric and symmetric vibrations appear at 1018 cm−1 and 803 cm−1, respectively. After the nanocoating is applied, these two peaks have clearly shifted to 1072 cm−1 and 788 cm−1 wavenumber, respectively. This suggests a clear change in electron density around O-Si-O bond after interacting with rubber surface [32]. Therefore, FT-IR data confirms that there are strong interactions between the coating and rubber film.

3.3. Bonding Mechanism between the Rubber Film and the Coating

The mechanism of the interactions between the nanocoating and the rubber film can be understood referring to the chemistry between the silica aerogel, silicone sealant, and the polychloroprene binder. Here, polychloroprene and phenol formaldehyde compatibilize the nanocoating onto the natural rubber film while silicone sealants containing methyltriacetoxysilane (MTAS) and ethyltriacetoxysilane (ETAS) act as coupling agents, binding the silica aerogel to the phenol formaldehyde unit of the binder.

Firstly, the coupling agents in silicone sealant and the silica aerogel are converted into their hydrolyzed state according to reaction mechanism shown in Figure 7. This process is enhanced by the presence of atmospheric moisture deposited on the natural rubber surface. The two coupling agents of silicone sealant, that is, MTAS and ETAS, will replace all of its Si-O-C bonds by Si-OH bonds.

Considering the structure of polychloroprene and phenol formaldehyde it is reasonable to argue that the OH groups of phenol formaldehyde interact with C-Cl group of polychloroprene forming a chemical bond with two matrices as shown in Figure 8. This argument is supported by the FT-IR data (Table 3) of cured polychloroprene and phenol formaldehyde resin. As given in the FT-IR data, peak due to C-Cl stretching frequency has disappeared after curing (Figure 6). Thus, it can be confirmed that a chemical change has occurred in C-Cl bond of polychloroprene. Furthermore, C=C stretching peak of polychloroprene has depleted after curing. It further suggests that electron density around C-Cl has changed due to the interaction with resin.

Binder before curingCorresponding vibrationBinder before curingCorresponding vibrationBinder after curingCorresponding vibration
IR frequency (cm−1)IR frequency (cm−1)IR frequency (cm−1)

690C-Cl stretching1450C=C benzene ring obscured by1018Single bond C-O stretching
882=C-H out of plane bending-CH2 methylene bridge1167C-O stretching
1018C-O stretching1504C=C aromatic ring1217Asymmetric stretch of phenolic
1045C-O stretching of CH2OH group1552C=C aromatic ringCH2-OH
1101C-C stretching1610C=C aromatic ring1303CH2 wagging
1153C-O stretching1700C=C stretching1362=C-H in plane bending
1189CH2 twisting2841C-H asymmetric stretching1425C=C benzene ring obscured by
1217CH2 twisting2850Out-of-phase stretching-CH2- methylene bridge
1237Asymmetric stretch of phenolicvibration of -CH21445C=C aromatic ring
CH2-OH2925CH2 in-phase stretching1540C=C aromatic ring
1300CH2 waggingVibration of -CH2- alkane1577C=C aromatic ring
1390O-H in plane3015=C-H stretching1657C=C aromatic ring
1340=C-H in-plane bending3400OH stretching2850Out of phase stretching
1428CH2 deformationVibration of -CH2-alkane
2917C-H asymmetric stretching
2954In-phase stretching vibration of
3306OH stretching

Step 1 (hydrolysis). The hydrolysis of silica aerogel, methyltriacetoxysilane (MTAS), and ethyltriacetoxysilane (ETAS) will produce hydroxyl groups on the silicone atom. These hydrolyzed compounds will further undergo polycondensation reaction.

Step 2 (polycondensation of the silicone sealant and silica aerogel). When the coating is cured, Si-O-Si bonds of all the materials will be formed through elimination of water molecules. This elimination happens during the curing process. The hydrolyzed MTAS and ETAS will be bonded to the phenol formaldehyde unit of the binder while natural rubber interacts through polymer-polymer interaction with the polychloroprene unit of the binder.

Compatibility of natural rubber and binder is controlled by the presence of Π-bond interactions between natural rubber and polychloroprene and the Π-bond interactions between natural rubber and benzene groups of phenol formaldehyde resin. Furthermore, the flat orientation of the phenolformaldehyde ring structure provides geometrically favorable arrangement for the nanocoating to be bonded to the rubber matrix. A possible mechanism is suggested in Figure 9.

3.4. SEM Characterization of Rubber Surfaces

SEM images of natural rubber and coated rubber surfaces are given in Figure 10. Both spray coated and dipped coated natural rubber films demonstrated a rough surface with a porous microstructure. The surface of the spray coated gloves appears to be rougher than the dipped coated surface due to the presence of nanosized particles embedded within the matrix. The particle size plays a major role in imparting superhydrophobicity to the coating, reducing the interfacial area between water droplets and the surface [7]. However, SEM images do not provide conclusive evidences regarding the best technique to obtain higher hydrophobic characteristics. Therefore, AFM characterization was carried out to understand the nanolevel morphological characteristics and surface roughness.

3.4.1. EDX Analysis of Superhydrophobic Nanocoating

EDX results confirmed the elemental composition of the nanocoating as O, C, and Si. According to the results summarized in Table 4 it is possible to conclude that the coating does not contain any fluorinated compounds. Moreover, the presence of high % of carbon confirms that the coating contains silica nanoparticles modified with an organic modifier.


C K28.96±1.4643.03
O K24.64±0.3527.49
Al K0.000.00
Si K46.40±0.1629.48
Si L

3.5. AFM Characterization of Rubber Surfaces

As shown in Figure 11, the three-dimensional surface of the spray coated rubber surface demonstrates sphere-like shapes in its topological image. Surface roughness of the spray coating has an average thickness of 100 nm and a root mean square roughness of 81 nm. A continuous coating is obtained when it is spray coated onto rubber surface where the roughness along the surface is not uniform. This increased roughness at nanoscale facilitates superhydrophobicity on the surface coating. According to Figure 12(b) the topology of dipped coating surface has a similar sphere shape appearance. The dipped coated rubber surface, however, does not have a continuous coating compared to spray coated gloves. In comparison to the spray coated surfaces, the dipped coated rubber surface has a relatively smooth surface morphology with an average thickness of 600 nm and root mean square roughness of 70 nm. This observation corroborates the contact angle measurements and, more importantly, the presence of thin and uniform layer on the spray coated rubber surfaces helps to retain the mechanical properties of the original rubber matrix.

3.6. Water Contact Angle (WCA), Sliding Angle (SA), and Durability of the Nanocoating

The initial water contact angle was 151° and 149° for spray coated and dipped coated gloves, respectively, while the uncoated gloves demonstrated a contact angle of 35°. Sliding angles for spray coated and dipped coated gloves were 7° and 8°, respectively. Durability of the coating was measured by recording the resulting WCA after each abrasion cycle (Table 5) as shown in Figure 13. A significantly durable coating was created when the spray coating method was used. Even after 40 cycles the change in WCA was insignificant.

Dipped coated gloveSpray coated glove
Number of cyclesContact angleNumber of cyclesContact angle


Data was not recorded after the superhydrophobic contact angle reached 85° in the dipped coated gloves.

The coated rubber films did not demonstrate oleophobic property as the oil droplets spread over the coated glove immediately after the contact. Similar observation was obtained when the coated rubber was contacted with low molecular weight organic solvents.

3.7. Permeability of Nanocoating towards Organic Solvents and Organic Acids

The permeation resistivity of the rubber films was tested against methanol and formic acid, since there is an increased demand for gloves which are dilute acid and low molecular weight solvent resistant. According to the NMR data (see supplementary data), spray coated gloves were resistant to methanol permeation for 40 min compared to 20 min for uncoated gloves. Even after 40 min there was no evidence of methanol penetrating through coated film confirming its significant resistivity against organic solvent penetration.

As shown by SEM images in Figure 14 there are no significant changes in the surface morphology of coated glove after exposure to methanol. This further confirms the argument given above. However, there was no significant resistivity towards formic acid.

4. Conclusions

Superhydrophobic coatings on natural rubber surfaces were successfully fabricated using modified silica nanoparticle dispersions. The films were prepared using both dipped and spray coating methods. The water contact angle of more than 150° was observed for the coatings. Sliding angles for spray and dipped coated gloves were 7° and 8°, respectively. However, according to the evidences obtained by AFM imaging, continuous and nanoporous coating with 100 nm thickness and root mean square roughness of 81 nm was observed for spray coated gloves, while the dipped coated gloves demonstrated high smoothness with a coating thickness of 600 nm and root mean square roughness of 70 nm in the surface. In addition, the mechanical properties were maintained compared to the uncoated rubber matrix when the coating was sprayed. In addition, the coating was durable even after being subjected to abrasion for a prolonged time. This observation together with the FT-IR characterization evidences suggests that there are strong interactions between the coating and the rubber surface. Interestingly, the coatings were significantly resistant towards methanol, suggesting its potential in low molecular weight solvent resistant applications.

Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this article.


Analytical support by Dr. Gayani Abeyaweera, Dr. Nuwan De Silva, and Mr. Eranda Karunarathna is acknowledged. The authors are also grateful to Kosala Lakmal and Eshan Malintha for engineering and technical support.

Supplementary Materials

Silica aerogel based superhydophobic nano-coatings for natural rubber surfaces. Figure 1: 13C NMR spectrum of polychloropene binder (solvent – CDCl3). Figure 2: 1H NMR spectrum of polychloropene binder (solvent – CDCl3). Figure 3: Methanol penetration detecting of the uncoated rubber films by exposing the uncoated ruuber film to methanol for 10, 20, 30 and 40 mins. Figure 4: Methanol penetration detecting of the coated rubber films by exposing the coated ruuber film to methanol for 10, 20, 30 and 40 mins.

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Copyright © 2017 Veromee Kalpana Wimalasiri et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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