Mohamed S. Selimab,
Sherif A. El-Safty*ac,
Maher A. El-Sockaryb,
Ahmed I. Hashemd,
Ossama M. Abo Elenienb,
Ashraf M. EL-Saeedb and
Nesreen A. Fatthallahe
aNational Institute for Materials Science (NIMS), 1-2-1 Sengen, Tsukubashi, Ibaraki-ken 305-0047, Japan. E-mail: sherif.elsafty@nims.go.jp; Web: http://www.nims.go.jp/waseda/en/labo.html
bPetroleum Application Department, Egyptian Petroleum Research Institute, Nasr City 11727, Cairo, Egypt
cGraduate School for Advanced Science and Engineering, Waseda University, 3-4-1 Okubo, Shinjuku-ku, Tokyo 169-8555, Japan. E-mail: sherif@aoni.waseda.jp; Web: http://www.nano.waseda.ac.jp/
dChemistry Department, Faculty of Science, Ain Shams University, Cairo, Egypt
eProcesses Development Department, Egyptian Petroleum Research Institute, Nasr City 11727, Cairo, Egypt
First published on 9th February 2015
Environmental concerns about the use of toxic antifoulants have increased the demand to develop novel, environmentally-friendly antifouling materials. Silicone coatings are currently the most effective non-toxic alternatives. This study focused on developing a model for silicone foul-release nanocomposites that were successfully designed, fabricated, characterized, and tailored toward foul-release (FR) coatings. A series of elastomeric polydimethyl-siloxane (PDMS)/Cu2O nanocube composites with different nanofiller concentrations was successfully synthesized, for the first time, as FR coatings via solution casting technique. Emphasis was given to the study of the physicomechanical and surface properties, as well as the easy release efficiency of the elastomer PDMS enriched with Cu2O nanocubes. The bulk properties of the nanocomposites appeared unchanged after adding low amounts of nanofillers. By contrast, surface properties such as contact angle and surface free energy were improved, and the settlement resistance and easy release behavior of the nanocomposites were enhanced. The surfaces were further proven to have reversible tunable properties and are thus renewable in water. The antifouling property of the nanocomposites was investigated by laboratory assays involving microfoulants such as Gram-positive and Gram-negative bacteria, as well as yeast organisms, for 30 days. Exposure tests showed that lower surface energy and elastic modulus of coatings resulted in less adherence of marine microfouling. The most profound effect recorded was the reduction of fouling settlement with nanofiller loadings of up to 0.1% Cu2O nanocubes. Thus, the good foul release and long-term durability confirmed that the present strategy was an attractive nontoxic and environmentally-friendly alternative to the existing antifouling systems.
The substantial environmental toxicity issues that surround the use of biocidal AF coatings have driven research in an environment-friendly direction with a particular focus on natural marine compounds and foul-release (FR) technology.10 Natural AF compounds also face regulatory hurdles with the estimated cost of assembling data packages on efficacy and environmental fate amounting to millions of dollars as well as with the timeline for the approval process.11
Non-stick, silicone FR coatings present a feasible, cost-effective alternative to biocidal AF coatings. Silicone coatings rely on a technology that acts in two ways: inhibiting the settlement of colonizing species and weakening their adhesion strength. By providing low-friction ultra-smooth surfaces, organisms that stick can be easily removed hydrodynamically ideally by simply bringing the ship to speed. These coatings do not leach and could be more durable than tin-free AF paints for certain vessel applications.12 Silicone polymers based on polydimethyl-siloxane (PDMS) have been the most promising FR coating system.13 The superior properties of PDMS FR coatings are due to their low surface energy, low surface roughness, low porosity, and high molecular mobility.14 The O–Si–O linkage, which presents water repellency, causes the good thermal stability, excellent resistance to oxygen, ozone, and UV light, anti-stickiness, and low chemical reactivity of the coating.15 Coatings based on silicone elastomers have inherently good FR properties; however, they require reinforcing additives (usually mineral fillers) to improve their specific properties and reduce the costs. This reinforcement can be achieved by incorporating inorganic nanoparticles (NPs) and conventional macro- and micro-scale composites because of the increased interaction at the polymer filler interface for the nanocomposites.16 The extent of nanocomposite property improvement depends on filler properties, concentration, morphology, degree of dispersion, and degree of adhesion with polymer chains.15,17
The use of NP-based metal oxide coatings represents a promising approach for the development of non-toxic control technologies for micro-fouling organisms. Surfaces can be engineered with low-surface energy coatings that minimize biological adhesion strength and allow FR with modest brushing/water spray pressures or with coatings that can prevent fouling through their photocatalytic activity. Metal oxide NPs are stable during contact with microorganisms.18 TiO2 NPs pose a greater potential than silica in minimizing biofouling on optical surfaces. In addition, techniques like nano-metal oxide coatings seem to be an effective method for combating fouling.19 Among them, Cu2O NPs are relatively easy to make, safe, and inexpensive, and the natural abundance of its source materials favors the fundamental and practical research on Cu2O.20
Cu2O NPs exhibit excellent antibacterial activity against Gram-positive and Gram-negative bacteria.18,21 A study has proven that surface hydrophobicity/super-hydrophobicity can be achieved on modified nano-Cu2O films,22 which showed potential for our field of application. A variety of interesting Cu2O nanostructures has been synthesized.23,24 Nanocubes represent one of the most important structural types of Cu2O because several other crystal morphologies of Cu2O (e.g., nanocages, octahedral, and more complicated structures) can be prepared through the shape transformation of Cu2O nanocubes.25 Furthermore, the antibacterial activity of cubic Cu2O NPs against Escherichia coli is superior to that of octahedral Cu2O NPs. The polar properties of the {100} crystal planes of Cu2O nanocubes are believed to perform an important function in the increased antibacterial activity.26
In the present work, a series of hybrid PDMS/cubic Cu2O nanocomposites was fabricated via solution casting technique for use as FR coatings. The surface properties were discussed based on the changes in water contact angle and surface free energy. New functions of Cu2O nanocubes were introduced here based on increasing the easy cleaning phenomena through raising hydrophobicity and lowering surface free energy that result in ultra-smooth surfaces with a mechanism that involves physical anti-adhesion. This research highlights the significance of the extent of dispersion of CuO2 nanofillers in determining the improvement in the physicomechanical and surface properties of the nanocomposites. Furthermore, AF performance was examined through biological assays to evaluate the nanocomposite FR behavior. The findings in this context are attractive for their merits such as simplicity, safety, environmental benignancy, commercial feasibility, and good potential for easy-cleaning systems.
The Fourier transform infrared (FTIR) spectra were recorded using a Nicolet iS10 (Thermo Scientific, USA) with 1 cm−1 resolution and 4000–400 cm−1 range. The samples were cast on potassium bromide (KBr) pellets (FTIR grade, Alfa Aesar, Karlsruhe, Germany). 1H NMR spectra were recorded on a Varian Mercury VXR-300 NMR spectrometer at 300 MHz (Varian, Inc., Palo Alto, CA, USA) using tetramethylsilane Me4Si (TMS) as internal standard and CDCl3 as the main solvent.
Particle size measurement based on the principles of dynamic light scattering (DLS) was performed using a Brookhaven Instruments 90Plus model nanoparticle size/zeta potential analyzer (USA). The accurate sizes of the NPs were analyzed by TEM because DLS gives hydrodynamic nanoparticle size. High-resolution transmission electron microscopy (HRTEM) was conducted with an electron microscope (JEM2100 LaB6, Japan) at 200 kV accelerated voltage and with 0.14 nm point–point resolution. In HRTEM, the solid sample was dispersed in ethanol solution using an ultrasonicator and then dropped on a copper grid coated with carbon film. Prior to inserting the samples in the HRTEM column, the grid was vacuum dried for 10 min. The nanocomposite samples for TEM analysis were prepared by ultra-cryomicrotomy with a Leica Ultracut UCT (Leica Microsystems GmdH, Vienna, Austria). Freshly sharpened glass knives with 45° cutting edges were used to obtain cryosections with approximately 100–150 nm thickness at −150 °C. The cross sections were collected individually in sucrose solution and directly supported on a 300-mesh copper grid.
X-ray diffraction (XRD) is a versatile and non-destructive technique that reveals detailed information about the chemical composition and crystallographic structure of natural and synthetic materials. XRD patterns were measured using a Panlytical X'pent PRO (Netherlands) with monochromated CuKα radiation with scattering reflections recorded for 2θ angle between 10° and 80° corresponding to d-spacing between 1.47 and 3.26 Å. To confirm the resolution of the diffraction peaks with standard reproducibility in 2θ (±0.005), the sample measurement was recorded using a monochromator and detector, which were used to generate focusing beam geometry and parallel primary beam. The standard diffraction data were identified according to the International Centre for Diffraction Data (ICDD) software with PDF-4 release 2011 database.
The optical micrographs of the samples obtained by mechanical mixing were recorded with an Olympus BH-2 microscope (Japan) where the images were obtained using Image J software program. Scanning electron microscopy images were obtained by a scanning electron microscope (JEOL JSM530). Before insertion into the chamber, the disk-like monolith substrates were fixed on the SEM stage using carbon tapes. Gold (Au) films were deposited on the substrates at RT using an ion sputter (EDWARDS S150). The distance between the target and the disk-like monoliths substrate was 5.0 cm. The sputtering deposition system used for the experiments consists of a stainless steel chamber, which was evacuated down to 8 × 10−5 Pa with a turbo-molecular pump backed up by a rotary pump. Before sputtering deposition, the Au target (4 in. diameter, 99.95% purity) was sputter cleaned in pure Ar. The Ar working pressure (2.8 × 10−1 Pa), the power supply (100 W), and the deposition rate were kept constant throughout the investigations. Moreover, to record the SEM images of the disk-like monoliths well, the SEM micrographs were operated at 20 keV.
SD (%) = ((Wf − Wi)/Wi) × 100 | (1) |
The total surface tension of a solid γtotalS is composed of three additive components: the Lifshitz–van der Waals dispersion component, γLWS, the polar electron-donor (Lewis base) component, γS−, and the polar electron-acceptor (Lewis acid) component, γS+ (eqn (2) and (3)):
![]() | (2) |
![]() | (3) |
Utilizing the surface tension γL of at least three different liquids of known components, two polar and one nonpolar, are necessary to obtain the three equations that can be solved for the unknowns of the solid, γLWS, γS+, and γS−. This research used diidomethane as the nonpolar liquid, and water and ethylene glycol were chosen as the polar liquids.
(i) Gram positive bacteria: Staphylococcus aureus, NCTC-7447 (Gram +Ve 1) and Bacillus subtilis, NCTC-1040 (Gram +Ve 2); (ii) Gram negative bacteria: Pseudomonas aeruginosa, NCTC-10662 (Gram −Ve 1) and Escherichia coli, NCTC-10416 (Gram −Ve 2); and (iii) yeast: Candida albicans, IMRU 3669.
Nutrient broth media were used for the cultivation and maintenance of the tested microorganisms. The nutrient broth composition (g L−1) was as follows: peptone, 5.0 g; NaCl, 5.0 g; yeast extract, 2.0 g; and beef extract, 1.0 g.30 Basal salt media were used for the weight loss and biodegradability tests. The foregoing media broth composition (g L−1) was as follows: potassium dihydrogen orthophosphate, 2.44 g; sodium dihydrogen orthophosphate, 5.57 g; ammonium chloride, 0.5 g; glycerol, 6.4 mL; magnesium chloride, 2.44 g; calcium chloride, 5.57 g; ferrous sulfate, 2.00 g; yeast extract, 0.1 g; and distilled water, 850 mL.31
Weight loss (mg cm−2) = ((Wbefore − Wafter)/time) | (4) |
%BD = ([WC − WS]/WS) × 100 | (5) |
In 2000, Wynne et al. evaluated two types of PDMS coatings, namely, the hydrosilation-cured and the condensation-cured PDMS, and found that the unfilled hydrosilation-cured PDMS has superior properties such as hydrophobicity, roughness, stability in water, non-shrinkage, and lower adhesion of barnacles compared with filled condensation-cured PDMS.37
Vinyl-terminated PDMS was obtained via anionic ring opening polymerization of D4 tetramer (because it is a less expensive and more readily available monomer) using a strong base catalyst (KOH), which is frequently used to ring open D4 at common polymerization temperatures of 140–160 °C (ref. 14 and 38) (see ESI, Scheme S1†). Siloxane dimers (tetramethyldivinylsiloxane) are usually used as end-capping reagents to control the molecular weight.39 After reaching equilibrium, the reaction is quenched by adding a strong acid (orthophosphoric acid). The conversion or polymerization rate of D4 is high at the beginning and then flattens out with time because of the decrease in monomer concentration during polymerization and because the living centers are enclosed by polymer chains in bulk polymerization.
The FTIR spectrum of the prepared vinyl-terminated PDMS sample revealed absorption bands at 2963 and 2905 cm−1 ascribed to asymmetric –CH3 stretching, at 1411 cm−1 assigned to –CH3 symmetric deformation, and at 1595 cm−1 assigned to Si–CHCH2 stretching absorption. The band at 1261 cm−1 corresponds to CH3 symmetric deformation, that at 1096 cm−1 to Si–O–Si asymmetric deformation, that at 866 cm−1 to Si–O–Si skeletal stretching, and that at 699 cm−1 to the symmetric stretching of the Si–C bond in –Si(CH3) group. The absence of any absorption peak at 2060 cm−1 and 3000–3500 cm−1 indicates the absence of any hydrosilane (Si–H) or hydroxyl groups (Si–OH) in the prepared polymer (see ESI, Fig. S1†).39a
The 1H nuclear magnetic resonance (NMR) spectrum distinguishes the signals of the chemical shift at 1.00 ppm caused by (Si–CH3) from those at 5.94–6.2 and 5.71–5.92 ppm by CH2CH–Si and CH2
CH–Si. The absence of a chemical shift at 4.6 ppm indicates the absence of Si–H and Si–OH linkages. The DSC sample was super-cooled at −130 °C and then heated from −130 °C to 50 °C with a glass transition (Tg) at −122 °C, cold crystallization at −95 °C, and melting (Tm) at −46 °C. A crystallization exothermal peak is observed during the cooling step and a single melting endothermic peak during the second heating step. The low Tg of silicones as reflected in their molecular mobility may contribute to their superior FR characteristics.39b
The curing of the prepared vinyl-terminated PDMS follows the hydrosilation curing mechanism where vinyl end-blocked polymers react with the SiH groups carried by functional oligomers. The addition occurs mainly on the terminal carbon and is catalyzed by organometallic compounds, preferably platinum metal complexes, to enhance their compatibility. This reaction has no by-product. Molded pieces made with a product from this curing mechanism are very accurate (no shrinkage). The mechanism of platinum hydrosilation (see ESI, Scheme S2†) was proposed by Chalk and Harrod,40 and the catalytic cycle has also been reported before.14
![]() | ||
Scheme 1 Preparation of Cu2O nanocubes (note: the picture on the right shows the crystal structure of Cu2O oriented to show {100} plane). |
The reaction mechanism can be summarized as follows: cupric sulfate could be dissolved in water and form a uniform ionic solution. When NaOH is added to the solution, Cu2+ reacts with OH− and forms blue insoluble Cu(OH)2. At RT, Cu(OH)2 is decomposed into cupric oxide and water. Ascorbic acid is then added as reducer to reduce cupric oxide (CuO) into Cu2O. In this process, NaOH serves not only as a reagent, but also for adjusting the pH of the solution.
The FTIR spectrum of the prepared Cu2O NPs revealed a strong absorption band at 626 cm−1 attributed to the Cu–O linkage of Cu2O, which agrees with previous literature.43 Therefore, the as-prepared products were pure Cu2O because no infrared-active mode of CuO around 530 cm−1 appeared (see ESI, Fig. S2†).
The high morphological uniformity of these Cu2O crystals is reflected in their XRD patterns shown in Fig. 1. The strong and sharp diffraction peaks suggest that the resultant products were well crystallized. The characteristic peaks for Cu2O (2θ = 29.69, 36.52, 42.41, 61.68, 73.61) marked by indices [(110), (111), (200), (220), (311)] showed that the resulting Cu2O was essentially crystalline. All the peaks of the prepared Cu2O NPs match well with that of standard Cu2O, and no diffraction peaks from metal copper or cupric oxide appear in the XRD patterns.
![]() | ||
Fig. 1 XRD pattern of the as-synthesized Cu2O nanocubes, inside DLS of the as-synthesized Cu2O nanocubes, and schematic of a liquid droplet on the surface of coated glass slide. |
The size of the Cu2O crystallites was estimated from the Debye–Scherrer eqn (6):
D = (Kƛ/β1/2)cos![]() | (6) |
DLS is a non-invasive technique that measures the size and size distribution of NPs dispersed in a liquid, as shown in Fig. 1. The size distribution profile of the synthesized NPs showed an average particle size of 90 nm. The polydispersity index of Cu2O NPs was 0.236, which indicates that the particles are polydispersed in nature. These results matched with the results from the XRD analysis.
The transmission electron microscopy (TEM) analysis (Fig. 2A–C) and SEM analysis (Fig. 2D) of the prepared Cu2O NPs showed that they have approximately uniform size, cubic shape, clean surface, and particle sizes between 70 and 110 nm. The inset shows the selected area electron diffraction (SAED) patterns (Fig. 2E) obtained by directing the electron beam perpendicular to the square faces of the cube. The square symmetry of this pattern indicates that each Cu2O nanocube was a single crystal bounded mainly by {100} facets. Furthermore, it exhibits individual NPs and clear lattice fringes with d spacing of 0.25 and 0.30 nm, corresponding to the {111} and {110} reflections of the cubic Cu2O structure, respectively (Fig. 2F).
The FTIR spectra of the PDMS/Cu2O nanocomposites provide evidence for the interaction between the polymer and the NPs. The shifts in the absorptions for Si–O–Si asymmetric deformation and Si–O–Si skeletal deformation are less vivid for low concentrations but are well observed when the nanofiller content was increased up to 5% loading. The peak for Si–O–Si asymmetric deformations shifts from 1034 cm−1 for vinyl-terminated PDMS to 1020 cm−1 for the nanocomposites, and the peak for Si–O–Si skeletal stretching shifts from 805 cm−1 to 792 cm−1 for the 5% loading sample. The increase in the intensity of the peak at 3500 cm−1, which is due to the OH stretching of the H-bond of the adsorbed water on the surface of Cu2O, did not appear at low concentrations but was observed on high filler loadings (see ESI, Fig. S3†).
The tensile modulus of the prepared nanocomposites is illustrated in Fig. 3. It is not affected by the incorporation of a small amount of Cu2O NPs (up to 0.1%) in the nanocomposites with an average value remaining at 3.6 ± 0.5 MPa. In other words, the stiffness of the silicone-based materials remains constant. A progressive increase of up to 8 MPa is observed for high concentrations (5% nanofiller loadings), which may be explained by aggregation and agglomerations that cause the increase in stiffness. For the PDMS/Cu2O nanocomposites and within the limited content of nanofillers (less than 0.5 wt%), the dynamic stress was unchanged with an average value of 1300 ± 185 Pa and then increased up to 3315.5 Pa (for the high content in Cu2O at 5 wt% nanofillers), which may be caused by the presence of aggregates at high concentrations.
Surface energy measurements on the PDMS/Cu2O nanocomposites were performed according to the van Oss–Chaudhury–Good (VOCG) model by measuring the surface contact angle with both polar (water, as in Fig. 4, and ethylene glycol) and nonpolar (diiodomethane) liquids, as shown in Table 1. The calculated surface free energy values of the unfilled and filled PDMS are summarized in Table 1. The results illustrate low surface free energy for the 0.1% Cu2O nanofillers and thus low adhesion of microorganisms. By contrast, the surface free energy gradually increases with increasing filler loadings of up to 5% because of the roughness caused by agglomerations and aggregation.
Sample design | θ Ethylene glycol | θ Diiodomethane | γtotalS (mN m−1) | Swelling degree in n-heptane (SD (%)) | |||
---|---|---|---|---|---|---|---|
Dry | Wet | Dry | Wet | Dry | Wet | ||
a Note: γtotalS calculated with van oss–Chaudhury–Good approach, Lifshitz–van der Waals component γLWS, lewise base component γS− and lewise acid component γS+. | |||||||
PDMS blank | 84° ± 2° | 78° ± 2° | 75° ± 1° | 70° ± 2° | 20.23 | 23.06 | 93.6 ± 1% |
PDMS/Cu2O (0.01%) | 95° ± 2° | 88° ± 3° | 80° ± 2° | 75° ± 3° | 17.85 | 21.32 | 90.3 ± 2% |
PDMS/Cu2O (0.05%) | 104° ± 3° | 97° ± 3° | 84° ± 2° | 79° ± 2° | 16.22 | 19.6 | 88.5 ± 1.5% |
PDMS/Cu2O (0.1%) | 120° ± 2° | 112° ± 2° | 89° ± 1° | 85° ± 2° | 14.096 | 16.39 | 89.9 ± 1% |
PDMS/Cu2O (0.5%) | 106° ± 1° | 96° ± 3° | 85° ± 1° | 80° ± 1° | 15.47 | 18.55 | 88.6 ± 2.6% |
PDMS/Cu2O (1%) | 98° ± 3° | 89° ± 2° | 81° ± 2° | 76° ± 2° | 17.37 | 20.2 | 88.4 ± 1.8% |
PDMS/Cu2O (3%) | 91° ± 2° | 87° ± 2° | 76° ± 2° | 72° ± 1° | 20.38 | 23.11 | 87.5 ± 1.2% |
PDMS/Cu2O (5%) | 83° ± 4° | 79° ± 4° | 71° ± 1° | 67° ± 2° | 23.31 | 31.31 | 85.9 ± 2.5% |
Swelling measurements represent a technique of choice for the characterization of the polymer network. This test consists of immersing a piece of composite in a good solvent (heptane) and monitoring the evolution of the swelling mass at regular intervals. The swelling degree of the filled PDMS was lower than that of the unfilled, as shown also in Table 1. A low swelling degree is typical of a more important crosslinking density. Thus, Cu2O NPs can be seen as additional (physical) cross-linking points, acting positively during network formation because of the excellent affinity between components.
Biodegradation can be defined as the process in which substances are broken down by the action of microorganisms. The microorganism's growth in the material increases the size of pores and induces cracks. As a result, the structure of the material is destabilized.47 The biodegradation of PDMS in natural or living organisms has been poorly examined.39 PDMS has been treated as nonbiodegradable and inert. At the turn of 1970s, the possibility of their biodegradation has been proven.48,49 Only few studies that focus on the biodegradation of various siloxanes have been reported. Nevertheless, the lack of studies did not affect the general assessment that polysiloxanes are a group of polymers that is difficult to biodegrade.49 In this work, AF and biodegradation analysis was performed on the prepared PDMS/Cu2O nanocomposites as follows.
Weight loss tests were carried out on the unfilled and filled PDMS nanocomposites from 0.1% PDMS/Cu2O (which was proven to enhance characteristics with low nanofiller loading of 0.01% and 0.05%, as described in the aforementioned tests) and up to 5% fillers. A comparison of the weight loss results of the unfilled and filled PDMS nanocomposites at various loadings were carried out and shown in Fig. 5A, which suggests that the weight loss is higher for the unfilled PDMS and decreased to nearly zero with 0.1% loadings in PDMS/Cu2O. As shown in Fig. 5B, the biodegradability percentages for 30 days were calculated, where the blends with low nanofiller concentrations degrade slowly, whereas those with high nanofiller concentrations degrade rapidly in 30 days. This finding indicated that the significant FR characteristics were found with design patterns that have well dispersion of Cu2O NP fillers at loading amount up to 0.1%. In such patterns, the Cu2O NPs may lead to increase surface area, chemical bonding, and surface smoothness of polymer-NPs surfaces (see Table S1†). Consequently, the enhancement in the surface properties and the adhesion resistance of microorganisms is achieved, thereby preventing surface deterioration. On the contrary, with the surface design patterns fabricated at high concentrations of up to 5% filler NPs, the gradual increase in the fouling adhesion is due to the agglomeration and aggregation of the NPs at high filler concentrations.
Generally, the resistance of Gram-negative bacteria toward antibacterial substances is related to the hydrophobic surface of their outer membrane rich in lipopolysaccharide molecules. The membrane acts as barrier to the penetration of numerous antibiotic molecules associated with the enzymes in the periplasmic space, which are capable of breaking down the molecules introduced from outside.50
The biofilm coverage on the surface of silicone was roughly determined through the biofilm formation images in the optical microscope for the unfilled and filled PDMS specimens before and after immersion in the used microorganisms, as shown in Fig. 6. For the unfilled PDMS, given that the silicone and glass slide are transparent, the picture background was white if no bacteria are attached to the silicone surface. The surface coverage of the dark area (fouled area) relative to the total area was assumed to be the surface coverage of the bacteria. The well-dispersed NPs observed, which are related to the low concentrations of Cu2O NPs up to 0.1%, were the reason for the homogeneity and immunity of the surface. By contrast, the non-homogeneity observed for the blank samples were due to the fouling settlement on its surface, which is observed for the characteristics achieved from the failure mechanism technique. With increasing nanofiller concentrations of up to 5%, the specimens were also densely fouled. The SEM micrographs for the unfilled and filled polymer nanocomposites (see ESI, Fig. S4†) were obtained and showed Cu2O NPs as white spots. A good dispersion and homogeneity of NP distributions is observed for concentrations up to 0.1%, thus affords improved surface characteristics and enhanced immunity against microorganisms. By contrast, additional loadings up to 5% of Cu2O NPs lead to aggregation and agglomerations and consequently increased surface roughness. Thus, air voids may be trapped between the agglomerates and reduce the surface properties and immunity of the coatings against fouling.
Footnote |
† Electronic supplementary information (ESI) available. CCDC 73304. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c5ra01597a |
This journal is © The Royal Society of Chemistry 2015 |