1. Introduction
Since Fujishima and Honda reported water splitting from titania electrodes [
1], the photocatalytic properties of titania nanomaterials have been widely studied in areas such as water splitting [
2,
3,
4], CO
2 conversion [
5], and organic pollutant degradation [
6,
7]. Many non-toxic, durable, resistant to reactions with chemical compounds, and cheap photocatalysis (TiO
2) have been widely studied regarding synthesis, properties, modification, and applications. Nanoscale titania combines the desirable properties of titania with the high surface areas achievable by nanomaterials. Although nano-titania has been used for various applications, its low absorption capability because of wide band gaps and charge recombination in the visible light region limits its use in solar power applications. Many studies have attempted to extend nano-titania absorption to the visible region using different approaches. Doping is a solution and success has been achieved using (noble) metal ions and several atoms [
8,
9,
10,
11].
Manipulation of dopant impurity and vacancy bands can improve the efficiency of photocatalysis in terms of mobility and diffusion rate. For example, theoretical study of Cu doping effect on TiO
2 was reported by density functional theory methods to simulate doped anatase (101) surface plane. Cu doping tends to extend surface-hole life times and increase photo exciton production through effective charge transfer and bandgap narrowing [
12]. Cl doping on rutile TiO
2 nanosheets produces light carriers leading to higher mobility for excitons. The photogenerated electrons and holes extend the lifetime of Ti
3+, which acts as an in situ cocatalyst [
13].
Another approach is the sensitization and semiconductor composite technique. Some dyes with redox properties and visible light sensitivity can be used in solar cells and photocatalytic systems [
14,
15]. Furthermore, the control effects of the surface properties, sizes, and shapes of titania nanoparticles were reported for increasing photocatalytic activity [
16,
17]. Mesoporous structure titania increases its light absorption ability because of increased surface area and improved particle light scattering. Moreover, improved light absorption ability enhances surface adsorption of reactants and reinforces photocatalytic activity [
18].
Structural dimensionality can also affect the photocatalytic performance and properties of titania materials. Various titania morphologies and structures (spherical particles [
19], nanorods [
20,
21], nanotubes [
22], and hollow spheres [
23,
24,
25]) were also studied to enhance the photocatalytic activity of titania nanoparticles. Although there are pros and cons regarding dimensionality, the zero-dimensional structure is better than the one-dimensional structure for the coating system. The one-dimensional structure needs an additional transfer process from ITO (Indium Tin Oxide)to the target substrate for the coating process. Moreover, it needs an arrangement for photocatalytic efficiency. Therefore, the zero-dimensional structure is desired for the coating application to the substrate. The zero-dimensional structure increases the size of the accessible surface area by achieving special structures such as whisker [
19] and hollow morphology [
24]. Overall, these increases result in better photocatalytic performance because the photocatalytic reaction is based on chemical reactions on the surface of the photocatalyst. Moreover, hollow structural features increase the light-harvesting capabilities of these materials because they enhance light use by allowing as much light as possible to access the interior [
23].
Titania hollow spheres can be synthesized using many approaches, including spraying [
26], soft and hard template [
27,
28], sacrificial template [
25,
29], and hydrothermal approaches [
30]. The template method is one of the most widely used ways to construct nanoarchitecture by adequate control of the nucleation and growth. The templates are generally divided into two groups such as hard template and soft template. The soft template approach uses aggregation structural features which are formed by inter and intra- molecular interaction force in the synthesis of nanoparticles. The hard template approach has the advantage of preparation of composite materials with different sizes and architecture under various requirements. In addition, this approach features high stability and reproducibility and can precisely control the dimension and specification of the target material. Metal–organic frameworks (MOFs) have widespread interest in the study of catalysis as hard template candidates due to their porous crystalline property and inherent characteristics toward catalysis. The MOFs are beneficial for highly uniform and tunable pore shape and size—the open pathway used as transport and diffusion [
27]. Photocatalytic CO
2 reduction performance to CH
4 was achieved by HKUST-1(Cu
3(BTC)
2)@TiO
2 due to efficient exciton transferal from TiO
2 to the MOF. The MOF provides promoted charge separation in TiO
2 and active sites for conversion of CO
2 [
28].
Polymer colloidal spherical beads are another commonly used approach in the template method. Titanium precursors are attached to the surface using a layer-by-layer method or sol-gel reaction. However, it is challenging to synthesize titania hollow spheres. Because of the high reactivity of titania precursors, the various methods have several disadvantages, such as the formation of irregular coatings, aggregation of the coated particles, and low efficiency of controlling the coating thickness. Therefore, it is necessary for the formation of dense, smooth titania coatings on the surface of polymer colloid particles to control the hydrolysis and diffusion rates of titania precursors in the reaction system. Controlling the reaction time is challenging because of the high reactivity of titanium precursors.
Typically, the hard template method for forming the core-shell-structured silica or titania particles tends to predominantly use a cationic polymer template. The hard template method involves the (1) preparation of hard templates, (2) functionalization/modification of the template surface to achieve favorable surface properties, (3) coating the templates with designed materials or their precursors using various approaches, possibly with post-treatment to form compact shells, and (4) the selective removal of the templates to obtain hollow structures. Some factors must be considered for the synthesis of well-controlled titania and polymer hybrid composites by in situ polymerizations, such as the (1) compatibility between titania and the polymer, (2) electrostatic attraction, and (3) acid-base interaction. In this study, we synthesized hollow titania spheres of various sizes using anionic modified polymer latex and a SiO2/carbon template as core materials using the Stöber method. The photoactivity of the produced particles was evaluated and applied to the paint to confirm the implementation of its capability.
Polymer films containing near-infrared (NIR)-reflective pigments receive attention for their potential applications in energy-saving fields. Organic dust in the air is easily adsorbed and adheres to the surface of these films, gradually reducing their NIR reflectance. Roofs of either white or a light color were cooler than their black counterparts because white has the best solar-reflective performance [
31]. However, white or light-colored roofs are readily contaminated by dust in the air, which gradually abates their NIR reflectivity [
32,
33,
34,
35]. To overcome the contamination, surface cleaning technology is required to attain sustainability, such as superhydrophobic surfaces that possess self-cleaning properties [
36,
37]. The removal of contaminants using photocatalyst particles onto the coating could be a candidate. Such a film can reduce the maintenance cost and guarantee equal performance of the IR reflective coating and is dust-proof.
One method for achieving high reflectivity is a multilayer design in which a low refractive index layer (
nL) and a high refractive index layer (
nH) are alternately stacked. Equation (1) gives an overview of the refractive index design of multilayer.
E represents the field strength, R is the reflectance, refl is the reflection, and inc is the incident. In the above equation, if n1 > n2, then the Erefl and Einc codes coincide, and constructive interference occurs. If n1 < n2, then the Erefl and Einc codes are opposite, so destructive interference occurs. Therefore, to achieve high reflectivity, n1 > n2, that is, when the coating layer is applied to the material, the refractive index of the coating layer should be higher than that of the material. A hollow structure is a method of applying the layered design of the refractive index. When hollow particles are introduced, the space inside is air (refractive index = 1), and ceramics, metal oxides, and polymers could be present on the outside. Since these materials have a higher refractive index than air, they can easily reflect light in the long-wavelength region. Furthermore, this method can increase the effectiveness of the insulation. The ceramic, metal oxide, and polymer layers on the outside have a lower thermal conductivity than steel grades used as materials; therefore, they reduce heat transfer because of thermal radiation, and the air inside has the lowest thermal conductivity, which is also great for reducing heat transfer.
In this paper we report that mesoporous hollow structured TiO2 nanoparticles were prepared using anionic modified acrylate polymer templates. The effect of acrylate modification on the uniform shell formation with rapid and unstable titania precursors was investigated. The photoactivity of the prepared nanoparticles was investigated using various organic dye materials, especially important properties for anti-contamination. Moreover, the effect of the phase fraction on the photocatalytic ability of the synthesized hollow titania nanoparticles was studied. Furthermore, the effects of the hollow structure were explored in terms of self-cleaning and heat shielding in IR reflective coatings. A suggestion for restraining surface contamination, which is one of the chronic problems of thermal insulation paints, and enhancing the thermal insulation performance was proposed to attain long-term sustainability.
2. Materials and Methods
2.1. Preparation of the Core Template
The top-down synthesis method was used to synthesize the core-shell-structured and hollow ceramic nanoparticles. Acid-containing core templates were prepared by seed emulsion polymerization using the Stöber method to provide better control over the particle size, produce more monodispersed particles, and minimize the possibility of forming a water-soluble polymer in an aqueous medium. Furthermore, 30 wt% methacrylic acid (99.5%, MAA Samchun Pure Chemical Co., Ltd., Seoul, Korea) was used as an acid functional monomer to make the particles alkali-swellable because of its distribution between the aqueous and monomer/polymer phases favors the latter more than acrylic acid.
For core template 1, the two-stage semi-continuous emulsion polymerization was performed in a 1000 mL, four-necked, round-bottom flask equipped with a paddle stirrer, a thermometer, a nitrogen gas inlet, a reflux condenser, and inlet tubes for the continuous feed of materials. Deionized water (430 g) and 10 wt% sodium dodecylbenzene sulphonate solution (SDBS, Sigma-Aldrich, St. Louis, MO, USA) (6 g) were added to the stirred flask while maintaining a nitrogen atmosphere. Then, a pre-emulsion mixture of styrene monomer (20 g, 99.5%, Samchun Pure Chemical, Seoul, Korea), DIW (10 g), and sodium persulfate (0.48 g, Tokyo Chemical Industry Co., Ltd., Tokyo, Japan) was immediately added to the flask and heated to 80 °C and kept for 30 min. Sequentially, a monomer mixture containing DIW (55.2 g), 10 wt% SDBS solution (2.76 g), and styrene monomer (110.4 g) was fed into the reactor at a rate of 3.74 g∙min−1, kept for 1 h, and cooled to room temperature. An additional process was conducted to increase the core latex size. As above, DIW (400 g) and the synthesized polystyrene core aqueous solution (40 g) were poured into a 1000 mL, four-necked, round-bottom flask with a stirrer, a thermometer, a nitrogen gas inlet, a reflux condenser, and inlet tubes for the continuous feed of materials. Sequentially, the solution was heated to 80 °C after injecting sodium persulfate aqueous solution (0.32 g in 8 g DIW). A pre-emulsion mixture of DIW (80 g), SDBS (2.2 g), styrene monomer (100 g), methacrylic acid (25 g), and ethylene glycol dimethacrylate (1 g, Tokyo Chemical Industry Co., Ltd., Tokyo, Japan) was fed into the flask at a rate of 4.07 g/min then, maintained for 1 h to produce an acrylate-modified polystyrene core template, and cooled to room temperature.
For core template 2, a four-neck flask containing DIW (201.6 g), ammonium nonylphenol ethersulfate (0.68 g, Rhodapex CO-436 from Rhodia, Brussels, Belgium), and ammonium persulfate (0.17 g, Sigma-Aldrich, St. Louis, MO, USA) was heated to 80 °C while maintaining a nitrogen atmosphere. A seed monomer mixture consisting of butyl acrylate (BA, 7.4 g), methyl methacrylate (MMA, 3.25 g), and methacrylic acid (MAA, 0.14 g) was rapidly charged into the flask and maintained for 1 h. The sodium persulfate aqueous solution (0.76 g in DIW 42.3 g) and ammonium nonylphenol ethersulfate solution (1.21 g in DIW 120.7 g) were then added to the flask. A monomer mixture of butyl acrylate (5.49 g, Samchun Pure Chemical, Seoul, Korea), methyl methacrylate (MMA, 78.8 g, Samchun Pure Chemical, Seoul, Korea), methacrylic acid (38.2 g), and hexanediol diacrylate (HDDA, 1.58 g, Tokyo Chemical Industry Co., Ltd., Tokyo, Japan) was fed into the reactor at a rate of 2.08 g/min, and the reaction temperature was lowered to room temperature after a 1 h reaction.
For core template 3, aqueous SDBS solution (0.2 g in 140 g DIW) and sodium persulfate (0.15 g in DIW) were added to the flask and heated to 80 °C. Styrene (3.2 g), SDBS (0.008 g), and water (1.6 g) were added to the flask for 1 min and maintained for 25 min at 80 °C. Styrene pre-emulsion (styrene (36.8 g), SDBS (0.092 g), and DIW (18.4 g)) was fed for 1 h, maintained for another 1 h, then cooled down to room temperature. In sequence, aqueous polystyrene latex solution (25 g in 198 g DIW) was added to the reactor, followed by 0.16 g SPS in 2 g of DIW. Monomer mixture pre-emulsion was fed for 1 h and maintained for another 1 h before cooling. The monomer mixture comprises MMA (35.9 g), MAA (14.9 g), HDDA (2.5 g), CO-436 (0.21 g), and DIW (40 g). Silica deposition was conducted using a modified Stöber method that involved the hydrolysis and condensation of tetraethyl orthosilicate (TEOS, Tokyo Chemical Industry Co., Ltd., Tokyo, Japan), a commonly used sol-gel precursor to amorphous silica. A desired amount of TEOS was added in batch or semi-batch mode to the core solution containing ammonia. In a typical synthesis, 2.5 g (30 wt%) of synthesized acrylate-modified polystyrene core solution was diluted with ethanol and deionized water. Under magnetic stirring, an ammonia solution was added to the batch reactor at room temperature. The TEOS and ethanol mixture solution was fed into the reactor at a rate of 0.57 g/min (feed time is 45 min). The reaction was conducted at room temperature for 8 h under stirring.
2.2. Preparation of Titania Hollow Spheres
Three different templates (two carbon templates (cores 1 and 2) and one SiO
2/carbon template (core 3)) were dissolved in ethanol (99.5%).
N,
N-Dimethylethanolamine (DMEA, 99%, Acros Organics, Waltham, MA, USA) or ammonia solution (28–30%, Samchun Pure Chemical Co., Ltd., Seoul, Korea) were added to the template-ethanol solutions under vigorous stirring for 30 min. Titanium tetrabutoxide (TBOT, 99%, Sigma-Aldrich, St. Louis, MO, USA) was quickly poured into the template-ethanol solutions. The template-ethanol solutions containing TBOT were stirred for 6 h. The core-shell-structured template particles coated with TBOT were separated by centrifuging, and the residue was discarded. The separated template particles were placed in a 60 °C convection drying oven for 1 day. Next, the core-shell-structured TiO
2 composite particles were gathered and calcined at varying temperatures from 400 to 800 °C for 2 h with an increase of 10 °C/min in air to obtain the hollow titania spheres.
Table 1 lists the detailed synthesis formulation.
2.3. Coating Application
Galvanized steel (POSCO) was degreased with surface-cleaning chemicals and deionized water. Synthesized hollow titania pigmented coating was applied to the steel for evaluating photocatalytic performance and the physical properties of titania. Solvent-borne thermal insulation paint (non-volatile ~40) of fluorine-based resin (Noroo paint & coatings, Anyang, South Korea) was applied on the galvanized steel using a bar applicator and cured at peak metal temperature (PMT) of 224 °C in a convection oven. The dry film thickness was measured using a portable thickness measurement system (Quanix 8500, Automation Dr. Nix, Köln, Germany), and the thickness was 25 μm. Hollow titania pigmented coating was prepared using the same paint as above by mixing pre-dispersed hollow titania solution in ethylene glycol dibutyl ether (non-volatile ~40).
For preparing the clear coating, the main binder was polyester resin (Skybon ES-960 from SK Chemical, Seongnam, Korea). Trixene-blocked isocyanate (BI7982 from Baxenden Chemicals Ltd., Lancashire, UK) was used as a curing agent. p-Toluenesulfonic acid (Nacure 2530 from King Industries Specialty Chemicals, Norwalk, CT, USA) and dibutyltin dilaurate (Sigma-Aldrich, St. Louis, MO, USA) were used as catalysts. Kokosol 150 (SK Chemical, Seongnam, Korea) was used as a solvent. A bar applicator was used to apply the coating to the substrate and the film was cured at PMT of 220 °C in a convective curing oven. Detailed formulation was summarized in
Table 2. The dry film thickness was measured using a portable thickness measurement system (from Quanix 8500, Automation Dr. Nix, Köln, Germany), and the thickness was 26 μm.
2.4. Characterization
The surface morphology of the synthesized titania (core-shell and hollow) was observed using scanning electron microscopy (SEM, Hitachi SU-6600, Tokyo, Japan) with an accelerating voltage of 20 kV. Before SEM observations, the samples were coated as pretreatment with 10-nm Pt/Pd. Transmission Electron Microscope (TEM, JEOL-2200FS, Tokyo, Japan) measurements were conducted using an image Cs-corrector with an accelerating voltage of 200 keV. The phase analysis and composi-tion determination of hollow titania was conducted using an X-ray diffractometer (XRD, D8 advance, Bruker AXS, Billerica, MA, USA) with CuKa radiation (0.154 nm). The Brunauer–Emmett–Teller (BET, BELSorp-Max, MicrotracBEL Corp, Osaka, Japan) surface area and Barret–Joyner–Halenda (BJH) pore size distribution measurements were conducted using N2 as the adsorptive gas. Various light responses of synthesized particles and pigmented steel sheets, such as light absorption performance in the UV region and light reflectance in NIR/MIR wavelengths, were measured using a UV–vis-NIR spectrophotometer (UV-3600 Plus, Shimadzu, Kyoto, Japan) with integrating sphere attachment (ISR-2600Plus, Shimadzu, Kyoto, Japan). Diffuse reflectance was measured by placing the measurement sample next to the reflectance measurement window on the side of the integrating sphere with a barium sulfate white plate as a standard to obtain the relative diffuse reflectance values.
The photocatalytic activity of the prepared titania particles was evaluated by degrading 20 mg/L methyl orange solution in a reservoir. Titania colloidal aqueous solution (0.5 g/L) was placed in the reservoir (50 mL). A photocatalytic degradation reaction under stirring was the conducted using UV irradiation after 30 min in the dark. The UV irradiation was provided by a 200 W mercury-xenon lamp (Execure 4000-d, Hoya candeo optronics Co., Saitama, Japan). Sampling was performed at regular intervals during the reaction. The residue concentration of methyl orange was calculated by measuring its absorbance at 460 nm using UV–vis-spectroscopy (UV-2501PC, Shimadzu, Kyoto, Japan) [
38]. The decomposition rate was calculated using the absorbance ratio to the initial absorbance value. Moreover, the photocatalytic activity observation of a hollow titania coated steel sheet was conducted in methylene blue solution (20 mg/L) under UV irradiation, as above. A coated steel sheet (50 mm × 50 mm) was prepared for the specimen. Methylene blue solution sufficiently covering the specimen surface was dropped on the steel sheet. Visual observation analysis was conducted at regular intervals under UV irradiation.
Particle migration (or colloidal stability) analysis in the solution was conducted using the Turbiscan lab (Lean on tech) for 10 min. The intensity of both transmitted and backscattered light covered the entire solution height when an emitted light, scattered by particles, passed through the sample solution. These intensities allowed the direct monitoring of local physical heterogeneities with a vertical resolution. Thus, the nascent destabilization phenomenon (sedimentation or creaming layers, aggregates, agglomerates, or coalescence) could be detected and monitored periodically at different intervals.
The thermal blocking performance of coating was evaluated using a modified ASTM D 4803 (standard test method for predicting heat buildup in polyvinyl chloride (PVC) building products) method under 250 W IR irradiation (IF-100, Philips, Amsterdam, Netherlands). A sealed Teflon box (160 mm × 160 mm × 250 mm, top-opened) with thermocouples was prepared instead of an open PVC box system of ASTM D 4803 (
Figure 1). A 150 mm × 150 mm coated steel sheet was placed on top of the box and sealed with Teflon. The temperature on the backside of the two coated steel sheet specimens was measured simultaneously to minimize environmental effects.
4. Conclusions
A study was conducted to prepare a novel hollow titania pigmented infrared reflective coating layer on steel substrate for better and prolonged performances. Surface contamination is a critical factor affecting the coating’s functionality and weatherability. Some functional paints, such as thermal barrier paints, dramatically decrease thermal control performance when organic pollutants, present in the atmosphere, are adsorbed on the coating surface.
This study used a hollow titania photocatalyst to achieve surface cleaning of the coating. It is more challenging to reveal the performance while the particles are in a binder rather than in a powder. When it presents near the coating layer, light can be easily absorbed, and contaminants adsorbed on the surface of the photocatalyst exhibit an adequate effect. Hollow structured titania was successfully produced and applied to the paint to achieve catalytic performance at 1-coat-1-bake. In this case, it is economically strengthened, and the unnecessary coating processes can be removed, so productivity is high. To manufacture the hollow particles, a direct chemical deposition method was used. Because the synthesis method proceeds in the heterophase, the titania precursor must be selectively formed on the target polymer template. A polymer template modified with MAA and titania with a core-shell structure were synthesized in the presence of a nitrogen-based base catalyst. At high pH, the polymer template has a negative charge on the surface by the carboxylate salt group, and the salt of the catalyst with a positive charge forms a salt on the polymer surface. The titania precursor is then selectively adsorbed to help the reaction.
To obtain a hollow structure, a process of removing the polymer core is required. In this study, heat treatment was conducted. The hollow titania particles formed as the heat treatment temperature was changed, confirming various A/R phase fractions. The different phase composition indicated another light absorption capability in a longer wavelength region, which is a critical characteristic of photocatalytic efficiency. In an organic decomposition test, CS1 particles (250 nm, calcinated at 700 °C) showed the best photocatalytic activity because of the proper phase composition between anatase and rutile. Furthermore, because of the hollow structure, it has a higher specific surface area than commercial photocatalyst particles, which means an increase in the active site, which is beneficial for improving photocatalyst efficiency.
The particle-pigmented coating also showed brilliant efficiency for both the removal of organic pollutants and the increase in IR reflectance. The particle floating tendency to the surface was examined, and the results show that hollow titania also promoted the performance of IR reflective coating.