# Release of Volatile Compounds from Polymeric Microcapsules Mediated by Photocatalytic Nanoparticles

Authors: J. Marques; L. F. Oliveira; R. T. Pinto; P. J. G. Coutinho; P. Parpot; J. R. Góis; J. F. J. Coelho; F. D. Magalhães; C. J. Tavares
Journal: International Journal of Photoenergy
 (2013)

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## Abstract

In this study we propose a suitable method for the solar-activated controlled release of volatile compounds from polymeric microcapsules bonded with photocatalytic nanoparticles. These reservoirs can find applications, for example, in the controlled release of insecticides, repellents, or fragrances, amongst other substances. The surfaces of the microcapsules have been functionalized with TiO2 nanoparticles. Upon ultraviolet irradiation, redox mechanisms are initiated on the semiconductor surface resulting in the dissociation of the polymer chains of the capsule wall and, finally, volatilization of the encapsulated compounds. The quantification of the output release has been performed by gas chromatography analysis coupled with mass spectroscopy.


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## Body

## 1. Introduction

Microencapsulation and release has been an area of growing interest in the last years due to the many application perspectives, like in pharmaceutical products for drug controlled release, such as of insulin and other proteins, or cosmetics [1–3]. Different approaches of microencapsulation have been reported in the last decade. The complex coacervation method is a technique that has been used to produce polymeric microcapsules [4, 5]. This process uses the interaction of different polymers with opposite charges to form insoluble complexes and originate a phase separation. The encapsulation is achieved by the deposition of such complexes around a hydrophobic core. Despite the simple fabrication and ease of use in time-release and thermal-release applications, this method presents a significant number of disadvantages like wide-size distributions, weak shell wall, and low kinetics of shell wall formation [6, 7]. Solvent evaporation is one of the most popular processes to achieve encapsulation. A core material, solid or liquid, and capsule wall material are mixed in a water-immiscible solvent and the resulting solution is emulsified in an aqueous solution [8, 9]. After solvent evaporation, the solid microcapsules are produced. However this method requires quite complex processes and is expensive. Hence, interfacial polymerization emerged as an easy method to prepare microcapsules. It allows a high degree of control over the physical/chemical properties using mild reaction conditions [10]. This method involves the condensation reaction between two monomers dissolved in immiscible solvents at the interface, creating a thin polymer film. Due to its intrinsic advantages, this method was used in this work and the relationship between the properties of the water/oil phase and the polymeric capsule wall was carefully studied. It is well known that the experimental conditions are an important factor for controlling shape, permeability, and physical properties of the microcapsule [11, 12]. Dodecane was used as oil phase and also as model organic volatile compound in which acyl chloride monomer was dissolved. An amine was dissolved in the water phase, resulting in the formation of polyamide film at the interface; as exemplified in Figure 1 [13].Figure 1
Scheme of the polymerization reaction.The immobilization of titanium dioxide nanoparticles in microcapsules can offer a wide range of practical applications and combines the main advantages of photocatalytic reactions with the possibility of controlled release by solar activation. These photoactive nanomaterials can be deposited onto several types of surfaces, including tents, curtains, and windows, amongst other surfaces [14]. Semiconductor photocatalysts have attracted a great deal of attention because of their potential applications for removing toxic organic and inorganic pollutants [15, 16].The main objective of this work was to produce polymeric microreservoir systems for the controlled release of volatile compounds (e.g., insecticides, deodorants, fragrances, etc.) upon solar activation. The TiO2 nanoparticles were synthesized by a modified sol-gel method and its microstructure was characterized by X-ray diffraction for different calcination temperatures. The controlled release of the encapsulated dodecane was studied in the presence of TiO2 catalysts with and without ultraviolet (UV) irradiation. In order to extend the semiconductor absorbance into the visible light region, aiming to reduce the semiconductor band gap, the TiO2 nanoparticles were doped with nitrogen anions [17].


## 2. Experimental

### 2.1. Materials

Titanium (IV) isopropoxide (>99%, Sigma-Aldrich), propyl alcohol (>98%, Sigma-Aldrich), triethylamine (>99%, Sigma-Aldrich), hydrochloric acid (37%, Sigma), poly(vinyl alcohol) (>98%, Sigma-Aldrich), ethylenediamine (>99.5%, Sigma-Aldrich), dodecane (>99%, Sigma-Aldrich), and sebacoyl chloride (>95%, Sigma-Aldrich) were used as received. Commercial TiO2 P25 powder was purchased from Degussa and used as reference photocatalytic material.


### 2.2. Synthesis of the N-Doped TiO2 Powders

The N-doped TiO2 nanoparticles were synthesized by a modified sol-gel method [18]. Triethylamine was used as nitrogen source for the attempted anionic doping of the TiO2 lattice. In a typical procedure, a solution was prepared with water and propyl alcohol (1 : 10) at pH 2.4 (adjusted by addition of HCl). N-doped TiO2 nanoparticles were prepared by dissolving 1 mL of titanium isopropoxide in 1.25 mL of solution under vigorous stirring followed by a dropwise addition of 3 mL of nitrogen precursor. The reaction was carried out under gentle stirring for two days to attain the particle doped with nitrogen.After the sol-gel synthesis, the N-doped TiO2 nanoparticles were collected by repeated centrifugation and washed with propyl alcohol. Amorphous powders were first annealed at 80°C in a conventional electric oven for 8 h and later calcined at 300°C, 500°C, 700°C, and 800°C during 2 h to produce nanometric powders. The resulting samples were named considering the calcination temperature as NP300, NP500, NP700, and NP800, respectively. The sample without any thermal treatment was identified as NPRT.


### 2.3.  Photocatalytic Activity

The photocatalytic oxidation of methylene blue (MB) in the presence of the N-doped TiO2 nanoparticles under UV irradiation was investigated in order to evaluate the photocatalytic activity at different calcination temperatures [19–22]. The same procedure was performed for the reference TiO2 P25 powder.In a typical experiment, 2 mg of photocatalyst was suspended in aqueous methylene blue solution (10−5 M) in a quartz cell (40 mm × 40 mm × 10 mm) at pH 7.2 [23, 24]. The suspension was irradiated with a high power LED source (Thorlabs, 700 mA) with an excitation centered at 365 nm (UV-A). The averaged irradiance was ~4 mW·cm−2.The absorbance of the MB was monitored at intervals of 5 min using a spectrophotometer (ScanSpec UV-Vis, ScanSci) in the range of 300–900 nm. The rate of photodegradation of MB was analyzed by monitoring the intensity variation of the main absorption peak at 665 nm.The kinetics of photocatalytic degradation of MB is a pseudo-first-order reaction and can be expressed according to the equation [24, 25]:
(1)ln(CC0)=-kt,
where C represents the dye’s concentration at the time t, which is proportional to its optical absorbance, and k is the first-order rate constant of the reaction.


### 2.4.  Detection of Hydroxyl Radicals

Photoluminescence technique (PL) was used for the detection of hydroxyl radicals (•OH) produced during the photocatalysis reaction. Coumarin was chosen as molecular probe, which readily reacted with •OH radicals to produce a highly fluorescent subproduct, 7-hydroxycoumarin (7HC), which shows a strong PL signal at 456 nm [26]. At room temperature, 5 mg of photocatalyst powder was dispersed in 4 mL of 10−3 M coumarin aqueous solution in a quartz cell (40mm×10mm×10mm). The pH was adjusted to 3.3 with a HCl 0.1 M solution. Initially, the coumarin solution with the modified N-TiO2 and reference P25 particles was kept in dark for 30 min to establish adsorption-desorption equilibrium. After this stabilization period, and at given intervals of UV irradiation, the suspension was centrifuged and then analyzed on a FluoroLog-3 fluorescence spectrophotometer with an excitation wavelength of 332 nm. The measurements were performed at room temperature and the emission and excitation slits were set to 2.0 nm.


### 2.5.  Polymeric Microcapsules

The microcapsules were prepared by using an adapted method based on interfacial polycondensation in an ultrasonic bath at a frequency of 30 kHz [13, 27, 28]. The encapsulation of dodecane into the microcapsules was achieved by the reaction between sebacoyl chloride and ethylenediamine, in presence of poly(vinyl) alcohol (PVA) as a surfactant. 415 μL (6.2 × 10−3 mol) of ethylenediamine was added to the 25 mL of the 2% PVA solution. In the organic phase, 1.5 mL of dodecane and 265 μL (1.2 × 10−3 mol) of sebacoyl chloride were added drop by drop to the previous solution. The water/oil emulsion was emulsified for 5 min under the same ultrasonic conditions followed by 5 minutes under magnetic stirring at 300 rpm. The resulting microcapsules were rinsed several times with deionized water to remove the unreacted amine.


#### 2.5.1. Characterization Methods

The gas chromatography coupled with mass spectrometry (GC-MS) analysis of dodecane output release from within the microcapsules was performed using a Varian 4000 Performance apparatus, equipped with a CP8944 VF-5 column and an ion trap mass spectrometer as detector. The carrier gas was helium, at a flow rate of 1 mL·min−1. Column temperature was initially 40°C, and then gradually increased to 270°C at 8°C·min−1. For GC-MS detection an electron impact ionization system was used with ionization energy of 70 eV.The crystalline structure of the photocatalysts was characterized by X-ray diffraction analysis (XRD, Bruker D8 Discover diffractometer) using Cu Kα radiation. The morphological properties of microcapsules were studied using a scanning electron microscope (SEM, NanoSEM-FEI Nova 200) at SEMAT/UM. Fourier-transform infrared spectroscopy (FTIR) of vacuum-dried microcapsules loaded with optimized N-doped TiO2 nanoparticles (at 30°C for 5 days) was performed at 132 scans and with a 4 cm−1 resolution between 500 and 4000 cm−1, using a JASCO 4200 FTIR spectrophotometer, operating in the ATR mode (MKII Golden Gate Single Reflection ATR System).


## 2.1. Materials

Titanium (IV) isopropoxide (>99%, Sigma-Aldrich), propyl alcohol (>98%, Sigma-Aldrich), triethylamine (>99%, Sigma-Aldrich), hydrochloric acid (37%, Sigma), poly(vinyl alcohol) (>98%, Sigma-Aldrich), ethylenediamine (>99.5%, Sigma-Aldrich), dodecane (>99%, Sigma-Aldrich), and sebacoyl chloride (>95%, Sigma-Aldrich) were used as received. Commercial TiO2 P25 powder was purchased from Degussa and used as reference photocatalytic material.


## 2.2. Synthesis of the N-Doped TiO2 Powders

The N-doped TiO2 nanoparticles were synthesized by a modified sol-gel method [18]. Triethylamine was used as nitrogen source for the attempted anionic doping of the TiO2 lattice. In a typical procedure, a solution was prepared with water and propyl alcohol (1 : 10) at pH 2.4 (adjusted by addition of HCl). N-doped TiO2 nanoparticles were prepared by dissolving 1 mL of titanium isopropoxide in 1.25 mL of solution under vigorous stirring followed by a dropwise addition of 3 mL of nitrogen precursor. The reaction was carried out under gentle stirring for two days to attain the particle doped with nitrogen.After the sol-gel synthesis, the N-doped TiO2 nanoparticles were collected by repeated centrifugation and washed with propyl alcohol. Amorphous powders were first annealed at 80°C in a conventional electric oven for 8 h and later calcined at 300°C, 500°C, 700°C, and 800°C during 2 h to produce nanometric powders. The resulting samples were named considering the calcination temperature as NP300, NP500, NP700, and NP800, respectively. The sample without any thermal treatment was identified as NPRT.


## 2.3.  Photocatalytic Activity

The photocatalytic oxidation of methylene blue (MB) in the presence of the N-doped TiO2 nanoparticles under UV irradiation was investigated in order to evaluate the photocatalytic activity at different calcination temperatures [19–22]. The same procedure was performed for the reference TiO2 P25 powder.In a typical experiment, 2 mg of photocatalyst was suspended in aqueous methylene blue solution (10−5 M) in a quartz cell (40 mm × 40 mm × 10 mm) at pH 7.2 [23, 24]. The suspension was irradiated with a high power LED source (Thorlabs, 700 mA) with an excitation centered at 365 nm (UV-A). The averaged irradiance was ~4 mW·cm−2.The absorbance of the MB was monitored at intervals of 5 min using a spectrophotometer (ScanSpec UV-Vis, ScanSci) in the range of 300–900 nm. The rate of photodegradation of MB was analyzed by monitoring the intensity variation of the main absorption peak at 665 nm.The kinetics of photocatalytic degradation of MB is a pseudo-first-order reaction and can be expressed according to the equation [24, 25]:
(1)ln(CC0)=-kt,
where C represents the dye’s concentration at the time t, which is proportional to its optical absorbance, and k is the first-order rate constant of the reaction.


## 2.4.  Detection of Hydroxyl Radicals

Photoluminescence technique (PL) was used for the detection of hydroxyl radicals (•OH) produced during the photocatalysis reaction. Coumarin was chosen as molecular probe, which readily reacted with •OH radicals to produce a highly fluorescent subproduct, 7-hydroxycoumarin (7HC), which shows a strong PL signal at 456 nm [26]. At room temperature, 5 mg of photocatalyst powder was dispersed in 4 mL of 10−3 M coumarin aqueous solution in a quartz cell (40mm×10mm×10mm). The pH was adjusted to 3.3 with a HCl 0.1 M solution. Initially, the coumarin solution with the modified N-TiO2 and reference P25 particles was kept in dark for 30 min to establish adsorption-desorption equilibrium. After this stabilization period, and at given intervals of UV irradiation, the suspension was centrifuged and then analyzed on a FluoroLog-3 fluorescence spectrophotometer with an excitation wavelength of 332 nm. The measurements were performed at room temperature and the emission and excitation slits were set to 2.0 nm.


## 2.5.  Polymeric Microcapsules

The microcapsules were prepared by using an adapted method based on interfacial polycondensation in an ultrasonic bath at a frequency of 30 kHz [13, 27, 28]. The encapsulation of dodecane into the microcapsules was achieved by the reaction between sebacoyl chloride and ethylenediamine, in presence of poly(vinyl) alcohol (PVA) as a surfactant. 415 μL (6.2 × 10−3 mol) of ethylenediamine was added to the 25 mL of the 2% PVA solution. In the organic phase, 1.5 mL of dodecane and 265 μL (1.2 × 10−3 mol) of sebacoyl chloride were added drop by drop to the previous solution. The water/oil emulsion was emulsified for 5 min under the same ultrasonic conditions followed by 5 minutes under magnetic stirring at 300 rpm. The resulting microcapsules were rinsed several times with deionized water to remove the unreacted amine.


### 2.5.1. Characterization Methods

The gas chromatography coupled with mass spectrometry (GC-MS) analysis of dodecane output release from within the microcapsules was performed using a Varian 4000 Performance apparatus, equipped with a CP8944 VF-5 column and an ion trap mass spectrometer as detector. The carrier gas was helium, at a flow rate of 1 mL·min−1. Column temperature was initially 40°C, and then gradually increased to 270°C at 8°C·min−1. For GC-MS detection an electron impact ionization system was used with ionization energy of 70 eV.The crystalline structure of the photocatalysts was characterized by X-ray diffraction analysis (XRD, Bruker D8 Discover diffractometer) using Cu Kα radiation. The morphological properties of microcapsules were studied using a scanning electron microscope (SEM, NanoSEM-FEI Nova 200) at SEMAT/UM. Fourier-transform infrared spectroscopy (FTIR) of vacuum-dried microcapsules loaded with optimized N-doped TiO2 nanoparticles (at 30°C for 5 days) was performed at 132 scans and with a 4 cm−1 resolution between 500 and 4000 cm−1, using a JASCO 4200 FTIR spectrophotometer, operating in the ATR mode (MKII Golden Gate Single Reflection ATR System).


## 2.5.1. Characterization Methods

The gas chromatography coupled with mass spectrometry (GC-MS) analysis of dodecane output release from within the microcapsules was performed using a Varian 4000 Performance apparatus, equipped with a CP8944 VF-5 column and an ion trap mass spectrometer as detector. The carrier gas was helium, at a flow rate of 1 mL·min−1. Column temperature was initially 40°C, and then gradually increased to 270°C at 8°C·min−1. For GC-MS detection an electron impact ionization system was used with ionization energy of 70 eV.The crystalline structure of the photocatalysts was characterized by X-ray diffraction analysis (XRD, Bruker D8 Discover diffractometer) using Cu Kα radiation. The morphological properties of microcapsules were studied using a scanning electron microscope (SEM, NanoSEM-FEI Nova 200) at SEMAT/UM. Fourier-transform infrared spectroscopy (FTIR) of vacuum-dried microcapsules loaded with optimized N-doped TiO2 nanoparticles (at 30°C for 5 days) was performed at 132 scans and with a 4 cm−1 resolution between 500 and 4000 cm−1, using a JASCO 4200 FTIR spectrophotometer, operating in the ATR mode (MKII Golden Gate Single Reflection ATR System).


## 3. Results and Discussion

### 3.1.  XRD Analysis

Figure2 shows the XRD patterns of the prepared N-doped TiO2 photocatalyst powders annealed at 300, 500, 700, and 800°C. The powders without calcination (curve a) exhibit an amorphous structure, with only minor traces of the most prominent anatase diffraction peaks. Therefore, the thermal treatment process is necessary to convert the amorphous TiO2 into a crystallized structure. For samples annealed at 300°C (curve b), clear diffraction peaks appear at 25.2° and 37.8°, which are attributed to (101) and (004) lattice planes of the anatase structure, revealing the formation of crystalline anatase phase at an early stage of the heat treatment; the peak observed at 35° is ascribed to Ti (100) planes. At this temperature no evidence of rutile phase is discerned. Moreover, upon increasing the calcination temperature, the intensity of these anatase diffraction peaks also increases. However, for the highest temperature of 800°C (NP800—curve e) the diffraction peak associated with the rutile phase (110) at 27.5° is more prominent, albeit lower than anatase preferential growth, indicating the starting transition of anatase phase to a more stable rutile phase. The diffraction pattern obtained for sample NP700 (curve d) is similar to the reference P25 material (not shown). The anatase average crystallite domain size varies very little with calcination temperature, increasing from 30 nm in its as-synthesized state to 50 nm for the highest temperature thermal treatment. At 800°C the rutile domain size is smaller than that corresponding to anatase, having a value of ~37 nm.Figure 2
XRD patterns of the N-doped TiO2 powders calcined at (a) room temperature (b) 300°C (c) 500°C, (d) 700°C, and (e) 800°C. A: anatase; R: rutile.


### 3.2.  Evaluation of the Photocatalytic Activity of the TiO2 Powders

#### 3.2.1. Adsorption of Methylene Blue on TiO2 Nanopowders

Comparative studies of the adsorption of methylene blue on the synthetized nanocatalyst powders were performed. A solution of methylene blue (10−5 M) was stirred with the different TiO2 nanoparticles (0.15 g·L−1) in the dark to ensure complete surface adsorption of dye. The change in methylene blue concentration was investigated by monitoring the maximum of absorbance of this dye at 665 nm, as plotted in Figure 3. An important change can be observed after 10 minutes, where the absorbance of methylene blue drops from 2.33 to values lower than 1.85, approximately 20% of the initial concentration value.Figure 3
UV-vis absorption variation at 665 nm measured in the dark of MB (10−5 M, pH 7.2) solution as a function of time for nano-TiO2 powders annealed at different temperatures. This experiment has also been performed for the P25 reference powder.These results indicate that the TiO2 nanoparticles strongly adsorb the methylene blue molecules at the surface. This can be explained by the pH effect on methylene blue/TiO2 nanoparticle suspensions. The pH of the solution influences significantly the characteristics of the TiO2 surface charge. Point of zero charge (PZC) is the value of pH at which the surface charge is zero. The knowledge of PZC of titania (PZC = 6.8) helps to predict the type and nature of the charge transfer that occurs preferentially. Since the photocatalytic assays were performed at pH higher than the reference PZC of titania, the surface of TiO2 nanoparticles has a negative charge and there is an electrostatic adsorption between negative-charged surfaces of TiO2 and methylene blue cations that carry a positive charge (2) [29–31]:
(2)TiOH+OH-⟷TiO-+H2O.
Thus, Figure 3 further indicates that 30 minutes was sufficient to reach the adsorption equilibrium between methylene blue and TiO2 nanoparticles. Therefore, for all photocatalytic experiments, the dye solutions with TiO2 nanoparticles were first stirred in the dark for 30 min before UV-A irradiation assays.


#### 3.2.2. Photocatalysis Assays

The photocatalytic reaction is very sensitive to the catalyst surface. The MB reacts with electrons and superoxide anions generated on the modified TiO2 particles under UV irradiation. The photocatalytic degradation reactions of MB on UV were investigated using the prepared N-doped TiO2 powders at different calcination temperature. In order to compare their UV light activities, the experiments were also carried out using the TiO2 powders without thermal treatment and the reference TiO2 P25 in the same way as using the N-doped TiO2. The evolution of MB concentration with time for each sample at 665 nm is presented in Figure 4.Figure 4
Photodegradation of MB (10−5 M, pH 7.2) solution as a function of UV-A irradiation time for TiO2 powders annealed at different temperatures and reference P25.The photocatalytic degradation is a pseudo-first-order reaction and its kinetics,k values (1), and the degradation (%) of MB showing the catalytic activity of each sample are given in Table 1. Although MB was quickly degraded during UV-A irradiation for all the nanoparticles with thermal treatment, it is evident that NP700 showed the highest photocatalytic activity. The increased photocatalytic efficiency of the powders annealed at higher temperatures can be related to the surface morphology and crystal structure. This effect is attributed to the higher content of the crystalline anatase phase for the samples calcined at 700°C compared to those at 300 and 500°C. According to the XRD results, the phase transformation from amorphous TiO2 to anatase was not complete at 300°C. At 800°C, some of anatase phase starts to transform to the more stable but photocatalytically less active rutile phase. The photolysis experiments (not shown), in the absence of TiO2 catalyst or samples without pre-treatment, revealed that the self-degradation of MB was almost insignificant under UV-A illumination.Table 1
Rate constant (k) and degradation (%) of the MB (10−5 M, pH 7.2) solution for TiO2 powders annealed at different temperatures.
Samples
k values (min−1)
Degradation (%) of MB solution after 120 min.
NPRT
—
2
NP300
1.6 × 10−3
16
NP500
6.0 × 10−3
40
NP700
2.4 × 10−2
95
NP800
1.5 × 10−2
85
TiO2 P25
1.7 × 10−2
88


### 3.3. Photoluminescence of Coumarin

Under ultraviolet irradiation the valence-band electrons of TiO2 are excited to conduction band, leading to the formation of photogenerated electrons (e−) and holes (h+) pairs. In aqueous medium •OH radicals are generated by the reaction between photogenerated holes and H2O. Related reactions may be summarized as follows:
(3)TiO2+hv→h++e-,O2+e-→O•2-,H2O+h+→O•H+H+.The detection by coumarin fluorescence is based on the fact that its hydroxylation generates various subproducts, in which only one is strongly fluorescent, 7-hydroxycoumarin, as follows:(4)Coumarin+O•H→7-Hydroxycoumarin.After the correction of the coumarin PL signal, which is almost negligible, the 7-hydroxycoumarin fluorescence signal can be used to determine the quantity of•OH generated in reaction. Figure 5 shows the changes of PL spectra from a coumarin solution with UV-A irradiation time in the presence of NP700. It is evident that a gradual increase in the fluorescence occurs over the time at ~456 nm. This signal can be related to 7-hydroxycoumarin and suggests that fluorescent product was formed during TiO2 photocatalysis due to the specific reaction between hydroxyl radical and coumarin. It is clearly seen in Figure 5(b) that the fluorescence intensity increases linearly with the irradiation time.(a) Photoluminescence spectra of coumarin solution (10−3 mol L−1, pH 3.3) after UV-A irradiation and (b) the time dependence of the photoluminescence intensity of 7-hydroxycoumarin at 456 nm, in the presence of the NP700 powder.
(a)
(b)In order to investigate the effect of temperature annealing on the formation rate of radicals, PL experiments were performed in same conditions of NP700 for all N-doped TiO2 prepared by sol-gel method. After 2 h of irradiation PL spectra were recorded and compared (Figure 6).Figure 6
Photoluminescence spectra of coumarin solution (10−3 mol L−1, pH 3.3) after 120 min of UV-A irradiation in the presence of N-TiO2 powders annealed at different temperatures.It is clear that the NP700 sample yields a higher PL intensity, implying a high formation rate of 7HC and•OH. It is interesting to note that the PL intensity decreased when NP800 was used. This can be explained by the fact that NP800 contains a two-phase mixture of anatase and rutile, which can be related to the increase of the recombination in photogenerated electrons and holes and subsequently block of •OH production on the TiO2 surface. The •OH formation rate on rutile phase is much lower than that on anatase phase. The observed PL signal was lower for calcined powders at temperatures below  700°C, meaning that a prominent anatase phase is directly correlated with enhanced •OH production.


### 3.4.  FTIR-ATR Analysis of Polyamide Microcapsules

The FTIR spectrum of the synthesized polyamide microcapsules functionalized with TiO2 is presented in Figure 7.Figure 7
IR spectra of microcapsules with TiO2 prepared by interfacial polymerization.Figure7 presents the absorption band related with –C=O stretching vibration of the secondary amide group at 1630 cm−1 and the corresponding N–H stretching vibration at 1544 cm−1, which shows the success of the interfacial polymerization, with formation of polyamide.The spectral region between 3500 and 3060 cm−1 corresponds to the –NH stretching vibration of the primary and secondary amines, which could be related to the excess of amine used. The large band at 3310 cm−1 is ascribed to the –C=O characteristic band. The peaks from 2970 cm−1 to 2830 cm−1 are attributed to the TiO2 showing that the nanoparticles were successfully adsorbed on the surface.


### 3.5.  SEM Analysis of Polymeric Microcapsules

Figure8 shows a SEM micrograph of the microcapsules (a) with N-doped TiO2 powders adsorbed onto polymeric wall and (b) microcapsule degradation upon UV-A irradiation. The resulting microcapsules have sizes ranging from 20–100 μm and spherical shape with a porous surface. The results presented in Figure 8(b) suggest that the microcapsule wall collapses after 2 h under UV-A irradiation. This can be related to the photocatalyst-driven oxidation-redution mechanisms that are developed on the catalyst surface and subsequent •OH radicals production that initiate the dissociation and subsequent breach of the polymeric wall.Scanning electron microscopy micrographs of dodecane-loaded polyamide microcapsules (a) with N-doped TiO2 nanoparticles adsorbed onto its surface and (b) microcapsule degradation upon UV-A irradiation.
(a)
(b)


### 3.6.  Evaluation of Dodecane Release by GC-MS

The GC-MS analysis of the UV-A-irradiated samples containing dodecane-loaded microcapsules adsorbed with TiO2 nanoparticles on the surface revealed the presence of dodecane as a principal compound from the output yield. In order to compare the results with a commercial sample of TiO2 P25, GC-MS experiments were performed only for the sample NP700, since it showed the best results in the photocatalysis and photoluminescence assays discussed before (Figures 4 and 6). Figure 9 shows the chromatograms obtained by GC-MS for irradiated microcapsules in the presence and absence of photocatalyst nanoparticles, while Figure 10 demonstrates the UV-A illumination effect on the output release of dodecane from within the aforementioned microcapsules adsorbed with the photocatalyst nanoparticles.Figure 9
Chromatograms obtained by GC-MS for UV-A-irradiated dodecane-loaded polyamide microcapsules in the presence and absence of N-doped TiO2 nanoparticles (NP700).Figure 10
GC-MS chromatograms obtained for dodecane-loaded polyamide microcapsules adsorbed with N-doped TiO2 nanoparticles (NP700), with and without UV-A irradiation.From the analysis of Figures9 and 10 it is demonstrated that the integrated area of dodecane peak is much higher when the microcapsules are adsorbed with the photocatalyst nanoparticles and under UV-A irradiation. These results strengthen the fact that under UV-A irradiation the surface of photocatalyst develops oxidation-reduction processes that originate the cleave of chemical bonds and thus the collapse of the polymeric capsule, yielding the release of the volatile compound (dodecane).Figure11 shows the output release concentrations in ppm of dodecane from the polyamide microcapsules, for different samples and experimental conditions. Due to the fact that these polymeric capsules may have some porosity, since the synthesis process is not fully optimized, it was found that dodecane can be released slowly either without the presence of the TiO2 nanoparticles or in its presence but without UV-A irradiation. The irradiation of the microcapsules with UV-A alone, in absence of titanium dioxide, is expected to degrade the polymeric wall, releasing the dodecane. However, upon the UV-A irradiation, the release rate of the volatile agent is much higher. The results obtained for the NP700 and TiO2 P25 confirm that nanoparticles prepared in this work present similar efficiency when compared with the commercial sample.Figure 11
Concentration (ppm) of the output release of dodecane (Dod) from the polyamide microcapsules, for different samples and experimental conditions.


## 3.1.  XRD Analysis

Figure2 shows the XRD patterns of the prepared N-doped TiO2 photocatalyst powders annealed at 300, 500, 700, and 800°C. The powders without calcination (curve a) exhibit an amorphous structure, with only minor traces of the most prominent anatase diffraction peaks. Therefore, the thermal treatment process is necessary to convert the amorphous TiO2 into a crystallized structure. For samples annealed at 300°C (curve b), clear diffraction peaks appear at 25.2° and 37.8°, which are attributed to (101) and (004) lattice planes of the anatase structure, revealing the formation of crystalline anatase phase at an early stage of the heat treatment; the peak observed at 35° is ascribed to Ti (100) planes. At this temperature no evidence of rutile phase is discerned. Moreover, upon increasing the calcination temperature, the intensity of these anatase diffraction peaks also increases. However, for the highest temperature of 800°C (NP800—curve e) the diffraction peak associated with the rutile phase (110) at 27.5° is more prominent, albeit lower than anatase preferential growth, indicating the starting transition of anatase phase to a more stable rutile phase. The diffraction pattern obtained for sample NP700 (curve d) is similar to the reference P25 material (not shown). The anatase average crystallite domain size varies very little with calcination temperature, increasing from 30 nm in its as-synthesized state to 50 nm for the highest temperature thermal treatment. At 800°C the rutile domain size is smaller than that corresponding to anatase, having a value of ~37 nm.Figure 2
XRD patterns of the N-doped TiO2 powders calcined at (a) room temperature (b) 300°C (c) 500°C, (d) 700°C, and (e) 800°C. A: anatase; R: rutile.


## 3.2.  Evaluation of the Photocatalytic Activity of the TiO2 Powders

### 3.2.1. Adsorption of Methylene Blue on TiO2 Nanopowders

Comparative studies of the adsorption of methylene blue on the synthetized nanocatalyst powders were performed. A solution of methylene blue (10−5 M) was stirred with the different TiO2 nanoparticles (0.15 g·L−1) in the dark to ensure complete surface adsorption of dye. The change in methylene blue concentration was investigated by monitoring the maximum of absorbance of this dye at 665 nm, as plotted in Figure 3. An important change can be observed after 10 minutes, where the absorbance of methylene blue drops from 2.33 to values lower than 1.85, approximately 20% of the initial concentration value.Figure 3
UV-vis absorption variation at 665 nm measured in the dark of MB (10−5 M, pH 7.2) solution as a function of time for nano-TiO2 powders annealed at different temperatures. This experiment has also been performed for the P25 reference powder.These results indicate that the TiO2 nanoparticles strongly adsorb the methylene blue molecules at the surface. This can be explained by the pH effect on methylene blue/TiO2 nanoparticle suspensions. The pH of the solution influences significantly the characteristics of the TiO2 surface charge. Point of zero charge (PZC) is the value of pH at which the surface charge is zero. The knowledge of PZC of titania (PZC = 6.8) helps to predict the type and nature of the charge transfer that occurs preferentially. Since the photocatalytic assays were performed at pH higher than the reference PZC of titania, the surface of TiO2 nanoparticles has a negative charge and there is an electrostatic adsorption between negative-charged surfaces of TiO2 and methylene blue cations that carry a positive charge (2) [29–31]:
(2)TiOH+OH-⟷TiO-+H2O.
Thus, Figure 3 further indicates that 30 minutes was sufficient to reach the adsorption equilibrium between methylene blue and TiO2 nanoparticles. Therefore, for all photocatalytic experiments, the dye solutions with TiO2 nanoparticles were first stirred in the dark for 30 min before UV-A irradiation assays.


### 3.2.2. Photocatalysis Assays

The photocatalytic reaction is very sensitive to the catalyst surface. The MB reacts with electrons and superoxide anions generated on the modified TiO2 particles under UV irradiation. The photocatalytic degradation reactions of MB on UV were investigated using the prepared N-doped TiO2 powders at different calcination temperature. In order to compare their UV light activities, the experiments were also carried out using the TiO2 powders without thermal treatment and the reference TiO2 P25 in the same way as using the N-doped TiO2. The evolution of MB concentration with time for each sample at 665 nm is presented in Figure 4.Figure 4
Photodegradation of MB (10−5 M, pH 7.2) solution as a function of UV-A irradiation time for TiO2 powders annealed at different temperatures and reference P25.The photocatalytic degradation is a pseudo-first-order reaction and its kinetics,k values (1), and the degradation (%) of MB showing the catalytic activity of each sample are given in Table 1. Although MB was quickly degraded during UV-A irradiation for all the nanoparticles with thermal treatment, it is evident that NP700 showed the highest photocatalytic activity. The increased photocatalytic efficiency of the powders annealed at higher temperatures can be related to the surface morphology and crystal structure. This effect is attributed to the higher content of the crystalline anatase phase for the samples calcined at 700°C compared to those at 300 and 500°C. According to the XRD results, the phase transformation from amorphous TiO2 to anatase was not complete at 300°C. At 800°C, some of anatase phase starts to transform to the more stable but photocatalytically less active rutile phase. The photolysis experiments (not shown), in the absence of TiO2 catalyst or samples without pre-treatment, revealed that the self-degradation of MB was almost insignificant under UV-A illumination.Table 1
Rate constant (k) and degradation (%) of the MB (10−5 M, pH 7.2) solution for TiO2 powders annealed at different temperatures.
Samples
k values (min−1)
Degradation (%) of MB solution after 120 min.
NPRT
—
2
NP300
1.6 × 10−3
16
NP500
6.0 × 10−3
40
NP700
2.4 × 10−2
95
NP800
1.5 × 10−2
85
TiO2 P25
1.7 × 10−2
88


## 3.2.1. Adsorption of Methylene Blue on TiO2 Nanopowders

Comparative studies of the adsorption of methylene blue on the synthetized nanocatalyst powders were performed. A solution of methylene blue (10−5 M) was stirred with the different TiO2 nanoparticles (0.15 g·L−1) in the dark to ensure complete surface adsorption of dye. The change in methylene blue concentration was investigated by monitoring the maximum of absorbance of this dye at 665 nm, as plotted in Figure 3. An important change can be observed after 10 minutes, where the absorbance of methylene blue drops from 2.33 to values lower than 1.85, approximately 20% of the initial concentration value.Figure 3
UV-vis absorption variation at 665 nm measured in the dark of MB (10−5 M, pH 7.2) solution as a function of time for nano-TiO2 powders annealed at different temperatures. This experiment has also been performed for the P25 reference powder.These results indicate that the TiO2 nanoparticles strongly adsorb the methylene blue molecules at the surface. This can be explained by the pH effect on methylene blue/TiO2 nanoparticle suspensions. The pH of the solution influences significantly the characteristics of the TiO2 surface charge. Point of zero charge (PZC) is the value of pH at which the surface charge is zero. The knowledge of PZC of titania (PZC = 6.8) helps to predict the type and nature of the charge transfer that occurs preferentially. Since the photocatalytic assays were performed at pH higher than the reference PZC of titania, the surface of TiO2 nanoparticles has a negative charge and there is an electrostatic adsorption between negative-charged surfaces of TiO2 and methylene blue cations that carry a positive charge (2) [29–31]:
(2)TiOH+OH-⟷TiO-+H2O.
Thus, Figure 3 further indicates that 30 minutes was sufficient to reach the adsorption equilibrium between methylene blue and TiO2 nanoparticles. Therefore, for all photocatalytic experiments, the dye solutions with TiO2 nanoparticles were first stirred in the dark for 30 min before UV-A irradiation assays.


## 3.2.2. Photocatalysis Assays

The photocatalytic reaction is very sensitive to the catalyst surface. The MB reacts with electrons and superoxide anions generated on the modified TiO2 particles under UV irradiation. The photocatalytic degradation reactions of MB on UV were investigated using the prepared N-doped TiO2 powders at different calcination temperature. In order to compare their UV light activities, the experiments were also carried out using the TiO2 powders without thermal treatment and the reference TiO2 P25 in the same way as using the N-doped TiO2. The evolution of MB concentration with time for each sample at 665 nm is presented in Figure 4.Figure 4
Photodegradation of MB (10−5 M, pH 7.2) solution as a function of UV-A irradiation time for TiO2 powders annealed at different temperatures and reference P25.The photocatalytic degradation is a pseudo-first-order reaction and its kinetics,k values (1), and the degradation (%) of MB showing the catalytic activity of each sample are given in Table 1. Although MB was quickly degraded during UV-A irradiation for all the nanoparticles with thermal treatment, it is evident that NP700 showed the highest photocatalytic activity. The increased photocatalytic efficiency of the powders annealed at higher temperatures can be related to the surface morphology and crystal structure. This effect is attributed to the higher content of the crystalline anatase phase for the samples calcined at 700°C compared to those at 300 and 500°C. According to the XRD results, the phase transformation from amorphous TiO2 to anatase was not complete at 300°C. At 800°C, some of anatase phase starts to transform to the more stable but photocatalytically less active rutile phase. The photolysis experiments (not shown), in the absence of TiO2 catalyst or samples without pre-treatment, revealed that the self-degradation of MB was almost insignificant under UV-A illumination.Table 1
Rate constant (k) and degradation (%) of the MB (10−5 M, pH 7.2) solution for TiO2 powders annealed at different temperatures.
Samples
k values (min−1)
Degradation (%) of MB solution after 120 min.
NPRT
—
2
NP300
1.6 × 10−3
16
NP500
6.0 × 10−3
40
NP700
2.4 × 10−2
95
NP800
1.5 × 10−2
85
TiO2 P25
1.7 × 10−2
88


## 3.3. Photoluminescence of Coumarin

Under ultraviolet irradiation the valence-band electrons of TiO2 are excited to conduction band, leading to the formation of photogenerated electrons (e−) and holes (h+) pairs. In aqueous medium •OH radicals are generated by the reaction between photogenerated holes and H2O. Related reactions may be summarized as follows:
(3)TiO2+hv→h++e-,O2+e-→O•2-,H2O+h+→O•H+H+.The detection by coumarin fluorescence is based on the fact that its hydroxylation generates various subproducts, in which only one is strongly fluorescent, 7-hydroxycoumarin, as follows:(4)Coumarin+O•H→7-Hydroxycoumarin.After the correction of the coumarin PL signal, which is almost negligible, the 7-hydroxycoumarin fluorescence signal can be used to determine the quantity of•OH generated in reaction. Figure 5 shows the changes of PL spectra from a coumarin solution with UV-A irradiation time in the presence of NP700. It is evident that a gradual increase in the fluorescence occurs over the time at ~456 nm. This signal can be related to 7-hydroxycoumarin and suggests that fluorescent product was formed during TiO2 photocatalysis due to the specific reaction between hydroxyl radical and coumarin. It is clearly seen in Figure 5(b) that the fluorescence intensity increases linearly with the irradiation time.(a) Photoluminescence spectra of coumarin solution (10−3 mol L−1, pH 3.3) after UV-A irradiation and (b) the time dependence of the photoluminescence intensity of 7-hydroxycoumarin at 456 nm, in the presence of the NP700 powder.
(a)
(b)In order to investigate the effect of temperature annealing on the formation rate of radicals, PL experiments were performed in same conditions of NP700 for all N-doped TiO2 prepared by sol-gel method. After 2 h of irradiation PL spectra were recorded and compared (Figure 6).Figure 6
Photoluminescence spectra of coumarin solution (10−3 mol L−1, pH 3.3) after 120 min of UV-A irradiation in the presence of N-TiO2 powders annealed at different temperatures.It is clear that the NP700 sample yields a higher PL intensity, implying a high formation rate of 7HC and•OH. It is interesting to note that the PL intensity decreased when NP800 was used. This can be explained by the fact that NP800 contains a two-phase mixture of anatase and rutile, which can be related to the increase of the recombination in photogenerated electrons and holes and subsequently block of •OH production on the TiO2 surface. The •OH formation rate on rutile phase is much lower than that on anatase phase. The observed PL signal was lower for calcined powders at temperatures below  700°C, meaning that a prominent anatase phase is directly correlated with enhanced •OH production.


## 3.4.  FTIR-ATR Analysis of Polyamide Microcapsules

The FTIR spectrum of the synthesized polyamide microcapsules functionalized with TiO2 is presented in Figure 7.Figure 7
IR spectra of microcapsules with TiO2 prepared by interfacial polymerization.Figure7 presents the absorption band related with –C=O stretching vibration of the secondary amide group at 1630 cm−1 and the corresponding N–H stretching vibration at 1544 cm−1, which shows the success of the interfacial polymerization, with formation of polyamide.The spectral region between 3500 and 3060 cm−1 corresponds to the –NH stretching vibration of the primary and secondary amines, which could be related to the excess of amine used. The large band at 3310 cm−1 is ascribed to the –C=O characteristic band. The peaks from 2970 cm−1 to 2830 cm−1 are attributed to the TiO2 showing that the nanoparticles were successfully adsorbed on the surface.


## 3.5.  SEM Analysis of Polymeric Microcapsules

Figure8 shows a SEM micrograph of the microcapsules (a) with N-doped TiO2 powders adsorbed onto polymeric wall and (b) microcapsule degradation upon UV-A irradiation. The resulting microcapsules have sizes ranging from 20–100 μm and spherical shape with a porous surface. The results presented in Figure 8(b) suggest that the microcapsule wall collapses after 2 h under UV-A irradiation. This can be related to the photocatalyst-driven oxidation-redution mechanisms that are developed on the catalyst surface and subsequent •OH radicals production that initiate the dissociation and subsequent breach of the polymeric wall.Scanning electron microscopy micrographs of dodecane-loaded polyamide microcapsules (a) with N-doped TiO2 nanoparticles adsorbed onto its surface and (b) microcapsule degradation upon UV-A irradiation.
(a)
(b)


## 3.6.  Evaluation of Dodecane Release by GC-MS

The GC-MS analysis of the UV-A-irradiated samples containing dodecane-loaded microcapsules adsorbed with TiO2 nanoparticles on the surface revealed the presence of dodecane as a principal compound from the output yield. In order to compare the results with a commercial sample of TiO2 P25, GC-MS experiments were performed only for the sample NP700, since it showed the best results in the photocatalysis and photoluminescence assays discussed before (Figures 4 and 6). Figure 9 shows the chromatograms obtained by GC-MS for irradiated microcapsules in the presence and absence of photocatalyst nanoparticles, while Figure 10 demonstrates the UV-A illumination effect on the output release of dodecane from within the aforementioned microcapsules adsorbed with the photocatalyst nanoparticles.Figure 9
Chromatograms obtained by GC-MS for UV-A-irradiated dodecane-loaded polyamide microcapsules in the presence and absence of N-doped TiO2 nanoparticles (NP700).Figure 10
GC-MS chromatograms obtained for dodecane-loaded polyamide microcapsules adsorbed with N-doped TiO2 nanoparticles (NP700), with and without UV-A irradiation.From the analysis of Figures9 and 10 it is demonstrated that the integrated area of dodecane peak is much higher when the microcapsules are adsorbed with the photocatalyst nanoparticles and under UV-A irradiation. These results strengthen the fact that under UV-A irradiation the surface of photocatalyst develops oxidation-reduction processes that originate the cleave of chemical bonds and thus the collapse of the polymeric capsule, yielding the release of the volatile compound (dodecane).Figure11 shows the output release concentrations in ppm of dodecane from the polyamide microcapsules, for different samples and experimental conditions. Due to the fact that these polymeric capsules may have some porosity, since the synthesis process is not fully optimized, it was found that dodecane can be released slowly either without the presence of the TiO2 nanoparticles or in its presence but without UV-A irradiation. The irradiation of the microcapsules with UV-A alone, in absence of titanium dioxide, is expected to degrade the polymeric wall, releasing the dodecane. However, upon the UV-A irradiation, the release rate of the volatile agent is much higher. The results obtained for the NP700 and TiO2 P25 confirm that nanoparticles prepared in this work present similar efficiency when compared with the commercial sample.Figure 11
Concentration (ppm) of the output release of dodecane (Dod) from the polyamide microcapsules, for different samples and experimental conditions.


## 4. Conclusions

A simple method was developed for the synthesis of a stable nanocrystalline N-doped TiO2 photocatalysts by a modified sol-gel method, which were adsorbed on dodecane-loaded polyamide-based microcapsules. The effect of annealing temperature on the photocatalytic activity of the nanoparticles under ultraviolet irradiation was investigated. It was found that photocatalytic activity of these nanoparticles is strongly dependent on the calcination temperature. The nanoparticles calcined at 700°C revealed the highest photocatalytic activity upon degrading methylene blue under UV-A irradiation. Furthermore, the formation of •OH radicals on the photocatalyst surface under UV-A irradiation was also monitored by fluorescence experiments. In the same way of MB degradation, the N-doped TiO2 powders calcined at 700°C form a higher number of hydroxyl radicals on its surface than powders annealed at lower and higher temperatures (800°C). This result can be related to the more stable and prominent anatase phase in this sample, in detriment to rutile formation at a higher temperature.This work has shown that polyamide based microcapsules with TiO2 adsorbed on the surface can be successfully used to trigger the release of a model organic volatile compounds by UV-A irradiation. By means of GC-MS experiments it was possible to identify and quantify the amount of volatile compound released.The proof of concept presented in this work can be extended to afford the preparation of microcapsules loaded with organic compounds that can be released in a controlled manner through UV-A irradiation.



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*Source: 712603-2013-03-04.xml*