K.
Katayama
*a,
Y.
Takeda
a,
K.
Shimaoka
a,
K.
Yoshida
a,
R.
Shimizu
a,
T.
Ishiwata
a,
A.
Nakamura
a,
S.
Kuwahara
a,
A.
Mase
b,
T.
Sugita
b and
M.
Mori
b
aDepartment of Applied Physics, Chuo University, 1-13-27 Kasuga, Bunkyo, 112-8656, Tokyo, Japan
bGraduate School of Engineering, Gunma University, 1-5-1 Tnejin-cho, Kiryu, Gunma 376-8515, Japan
First published on 13th January 2014
Two analytical methods for the evaluation of photocatalytic oxidation and reduction abilities were developed using a photocatalytic microreactor; one is product analysis and the other is reaction rate analysis. Two simple organic conversion reactions were selected for the oxidation and reduction. Since the reactions were one-to-one conversions from the reactant species to the product species, the product analysis was simply performed using gas chromatography, and the reactions were monitored in situ in the photocatalytic microreactor using the UV absorption spectra. The partial oxidation and reduction abilities for each functional group can be judged from the yield and selectivity, and the corresponding reaction rate, while the total oxidation ability can be judged from the conversion. We demonstrated the application of these methods for several kinds of visible light photocatalysts.
In most of the applications of photocatalytic reactions, only the oxidation ability, especially total oxidation from organics to carbon dioxide and water, has attracted attention. However, photocatalysts also have the abilities of partial or selective oxidation,2–7 and reduction8–10 for various aromatic compounds.11,12 Selective oxidation of the alcohol functional group gave a high yield.13 The reaction mechanism of the reduction of nitro compounds was investigated in detail,8,14,15 and imine formation was reported after reacting with alcohols.16 Furthermore, complicated reactions involving the photocatalytically generated intermediate radical species were also observed.5,17,18
In recent years, the demand for visible light responsive materials has been increasing, and many papers on the development of new materials have been published. This is not only for organic decomposition, but also for generation of solar fuels and light harvesting applications.19–21 Although the development of materials has been intensively explored, the analytical methods for understanding the abilities of the materials have not changed. Typical methods of examining photocatalytic materials are the color degradation of methylene blue in aqueous solutions22,23 and the decomposition of acetaldehyde under ambient conditions,24 defined in the Japanese Industrial Standard (JIS). These methods give information on total oxidation ability. There is another promising method, where the oxidation of dimethylsulfoxide is observed by ion chromatography.25 Since methyl groups are replaced with hydroxyl radicals in a stepwise manner, the obtained products provide direct information on the hydroxyl radical activity.
From our point of view, the analytical methods for photocatalysts are not sufficient to cover many recently developed materials, which may have other potential applications. The problems with the conventional analytical methods are as follows: (1) under aqueous or ambient conditions, various AOSs, depending on the experimental conditions (pH, humidity, coexisting species), are involved in photodecomposition, and it is difficult to determine which one is the actual cause of the reaction; (2) methylene blue is not a good test material for dye degradation because it is subject to multi-point reactions in the molecule at the same time, as we clarified in a previous study,26 and the color degradation does not necessarily reflect the total oxidation ability.
We recently developed a spectroscopic monitoring system for photocatalytic reactions using a microreactor26 to reduce the reaction time, and successfully accomplished the quick monitoring of a photocatalytic reaction in a capillary. There are also several other reports on the decrease in reaction time by utilizing microreactors in photocatalytic reactions.27–32 We studied the reaction mechanisms for various dyes composed of different main structures, and we successfully performed a kinetic analysis and clarified multi-step reactions, self-catalytic reactions, and more complicated reactions by monitoring the intermediate species involved in each reaction. The results suggested that typical analyses based on the quasi-first-order or Langmuir–Hinshelwood mechanisms33,34 are not sufficient to clarify the reaction processes correctly. Furthermore, we proposed a new concept of a photocatalytic microreactor, in which no electrical resources are necessary to perform the photocatalytic reaction due to the use of a natural force such as capillary force or diffusion due to the concentration gradient, and successfully demonstrated its use in our previous paper.35
In this study, we propose a new methodology to clarify the actual abilities of photocatalytic materials, by obtaining the selective oxidation, reduction and total oxidation abilities and the corresponding reaction rates through simple screening methods using a photocatalytic microreactor. We performed some of the oxidation and reduction reactions in organic solvents, not in water, to avoid complex reactions involving various AOSs. By analysing the simple oxidation and reduction reactions, the electron or hole donation abilities can be understood. We applied two methods for these reactions; one is product analysis to obtain the conversion, yield and selectivity, giving information on the total oxidation, partial oxidation and reduction abilities, and the other is reaction rate analysis by monitoring the reaction directly inside the microreactor using UV spectra.
The photocatalyst was coated inside a fused silica capillary (I.D. 1.1 mm, O.D. 1.4 mm) with a length of 6 cm. The capillary was transparent, and was treated using an alkaline solution before coating. The capillary was soaked in paste, filled with the solution three times, and heated to 450 °C in a furnace for 1 h. Six capillaries were bundled together, and were placed in a test tube containing a reactant solution (1 mL). Due to the capillary force, the reactant solution typically rose a few centimeters above the solution surface.
The test tubes were loaded onto a merry-go-round type photoreaction stage with 8 test tube holders (Fig. S2†), and a light was shone from the side at a distance of about 10 cm, typically for 18 h. The reaction time was decided in advance by checking the necessary reaction time for 1 mL of a reactant solution with 6 photocatalytic microreactors. A UV-LED with a wavelength of 365 nm and an intensity of 360 mW cm−2 was used as a UV source, and a quasi sunlight source (XC-100, Solax) was used as a visible light source. After the reaction, the solution was analysed using gas chromatography (Shimadzu, GC-2014) and GC mass spectrometry (Agilent, 6890N(GC), 5975B (inert XL El/Cl MSD)).
For the reaction rate analysis, a reaction monitoring system was used (Fig. S3†), which was developed in our previous paper for studying the dye degradation processes.26 Some modifications were made to measure the UV spectra of simple organic molecules. The light source was a deuterium lamp (D2), and a UV spectrometer (Ocean optics, USB4000) covering a wavelength range of 220–400 nm was used. The capillary used for the photocatalytic microreactor was made of fused silica with a diameter of 500 μm.
The solution was injected into the capillary using a syringe pump. After the flow stopped, we waited for ca. 30 seconds until adsorption equilibrium was reached. The photocatalytic reaction was initiated by light irradiation from the top side. The light sources were UV-LEDs at 365 nm and 450 nm for UV photocatalysts and visible light photocatalysts, respectively. Perpendicular to the light, a fiber tip connected to the D2 lamp was placed at the reaction location. The other end of the fiber tip was placed on the opposite side of the D2 lamp, and the absorption spectrum was monitored with a spectrometer. The intensity of the D2 lamp was adjusted so as not to induce photoreactions or photocatalytic reactions.
As a typical photocatalyst, TiO2 powder (P25, average diameter (D): 21 nm) was used. It was mixed with water (3.33 mL) and acetylacetone (0.33 mL) in a mortar for 30 min, to prepare a TiO2 paste. A tungsten oxide coating solution (Toshiba materials, SJ9003-1, D: ca. 100 nm), nitrogen doped titanium oxide (N–TiO2, D: 22 nm), N–TiO2 doped with silicon (N–Si–TiO2, D: 11 nm), which is effective for reducing the defects in TiO2, and N–Si–TiO2 deposited with vanadium (V–N–Si–TiO2, D: 13 nm),36,37 for which enhanced photocatalytic ability was reported, were used as visible light photocatalysts. Powder samples were dispersed in a solution using the same method as for the TiO2 powder to prepare a paste. The method for the paste preparation is a general procedure for coating a nanoparticulate inorganic material on a glass. For all materials used here, it was confirmed that the thickness of the coating was 3 ± 0.5 microns, but the porosities ranged from 40 to 60%.
We investigated the organic conversion of various molecules due to photocatalytic reactions, and we selected the following reactions as candidates to show the oxidation and reduction abilities. To select the reactions, we placed importance on the simplicity of the reactions and easy monitoring of the UV spectra of the reactants and products.
The oxidation of benzyl alcohol (BAlc) to benzaldehyde (BAld)2,5 and the reduction of BAld to BAlc were selected, and the reaction schemes are shown in reactions (1) and (2) (Scheme 1). They are the reverse reactions of each other, and they can be controlled simply by changing the solvent: acetonitrile for oxidation and ethanol for reduction. For the oxidation, holes are used as an oxidant. Electrons are used for reduction since ethanol is a good scavenger of photoexcited holes, which prevents the recombination of electrons.14,38 Initially, we chose these reactions because the product analyses by GC and the monitoring of the spectra were easy, as we only had to monitor BAlc and BAld. However, we selected another reduction reaction, the reduction of nitrobenzene (NB) to aniline (AN) (reaction (3), Scheme 1),8,14,15 due to several reasons which we will explain in the following section.
The conversions, yields, and selectivities are summarized in Table 1. The conversion values can be used as a guide for estimating how efficiently the photoexcited electrons and holes were utilized, namely the total oxidation ability. The selectivities and yields are indicators of how many electrons and holes were used for the intended reactions.
Entry | Conversion (%) | Yield (%) | Selectivity (%) |
---|---|---|---|
(1) | 24 | 8 | 33 |
(2) | 69 | 23 | 33 |
(3) | 6 | 5 | 77 |
The concentration changes during the reactions are shown in Fig. 3. An increase in the concentration of BAld and a decrease in the concentration of BAlc were confirmed and the change was gradually saturated after about 60 s. It was noted that the sum of the BAld and BAlc concentrations remained at 5 mM. This indicated that this reaction proceeded with 100% selectivity until 60 seconds after the reaction started. We suppose that the reaction was saturated because the product species covered the active reaction sites, since the reactivity was recovered by replacement of the solution.
Furthermore, the concentrations of BAld and BAlc showed linear changes with time, and this indicated that this reaction is zeroth order, which can be explained by the rate analysis of the surface reaction (see Appendix). Since the reaction became saturated as it proceeded, the straight parts of the concentration curves were used to analyse the data. We successfully obtained a reaction rate constant of 0.011 mol L−1 s−1.
Similarly, the reduction of BAld was monitored as shown in Fig. 2(b). The reduction did not proceed until 60 s after the photoirradiation, and the concentration of BAld suddenly decreased after that. We tried fitting the spectrum in a similar way as for the oxidation reaction, but it was very difficult to obtain the exact concentration of BAlc because the absorption intensity of BAld is much stronger than that of BAlc for the same concentration, therefore the contribution of BAlc to the spectrum was difficult to deduce, and the error was very large for the smaller concentration of BAlc, as shown in Fig. 3(b). (It is noted that the absorbances of BAld and BAlc in Fig. 2(a and b) were different because of the different solvents.) Since it is still unclear why there was a lag time for the start of the reaction and the accuracy of the BAlc concentration was not good enough, we selected another reaction for the reduction reaction.
Then, we used the conversion of NB to AN, which is a well-known reduction reaction that proceeds via photocatalysis. The peak at 270 nm, corresponding to NB, gradually decayed and a new peak at 250 nm appeared. The reaction was saturated after approximately 100 s. However, the spectrum of the product did not perfectly match that of AN, which shows a peak at approximately 240 nm.
We suspected that AN was subject to photoreaction, and thus the change in the spectrum of AN on irradiation with UV light was monitored. Actually, the peak in the spectrum shifted from 240 to 250 nm and the resulting spectrum agreed well with the spectrum of the product of the NB reduction. The product was an imine compound, as confirmed by the GC-MS analysis (N-ethylideneaniline). Thus, it was considered that AN was generated in the reduction of NB but that the generated AN was changed into the imine compound by reacting with the acetaldehyde generated via the oxidation of ethanol.
However, we found out that AN did not react when 2-propanol was used as a solvent, probably because the oxidized molecule, acetone, did not react with AN. The absorption spectra for the reduction of NB in 2-propanol are shown in Fig. 2(c), and we could successfully observe the pure reduction reaction of NB to AN. The spectra obtained during the reaction were fully fitted to combinations of the AN and NB spectra (Fig. S4(c)†). The concentration change during the reaction is shown in Fig. 3(c). We observed that the reaction started after 10–20 s, which was much shorter than the corresponding time for the reduction of BAld, and the lag time was reproducible as long as TiO2 was used. Neglecting the lag time, the concentration change corresponded to a 1st order reaction, as shown in Fig. 3(c), and a reaction rate of 0.032 s−1 was obtained. (It is noted that this value is the reaction rate multiplied by the adsorption equilibrium constant. See Appendix.)
The results for the oxidation reaction of BAlc are shown in Table 2. The corresponding results for TiO2 under UV irradiation of similar intensity are shown too. Overall, the oxidation abilities of the visible light photocatalysts were comparable to that of TiO2 under UV illumination, considering differences in the light intensity and the absorbance of the materials, etc. WO3 showed the highest conversion, but the selectivity was quite low. With regard to the Si doping, N–Si–TiO2 showed higher conversion and selectivity compared with N–TiO2. Vanadium deposition gave a lower efficiency for the oxidation. The results for the reduction reaction of BAld are shown in Table 3. Compared with TiO2, the reduction abilities of the visible light photocatalysts were quite low on the whole, and no reduction product was observed for WO3, which can be explained by the low conduction band position. For the visible light photocatalysts, N–Si–TiO2 showed the highest conversion and selectivity, and vanadium deposition lowered the reaction efficiency.
Entry | Conversion (%) | Yield (%) | Selectivity (%) |
---|---|---|---|
TiO2 with UV | 17 | 3.7 | 22 |
WO3 | 25 | 0.3 | 1.0 |
N–TiO2 | 7.5 | 3.7 | 49 |
N–Si–TiO2 | 14 | 8.1 | 56 |
V–N–Si–TiO2 | 8.8 | 5.6 | 56 |
Entry | Conversion (%) | Yield (%) | Selectivity (%) |
---|---|---|---|
TiO2 with UV | 51 | 17 | 17 |
WO3 | 8.3 | 0 | 0 |
N–TiO2 | 14 | 2.4 | 17 |
N–Si–TiO2 | 18 | 5.2 | 29 |
V–N–Si–TiO2 | 12 | 1.6 | 13 |
A reaction rate analysis was performed for the visible light photocatalysts. Since they showed very low reduction abilities, we studied only the BAlc oxidation reaction, which proceeded with almost 100% selectivity even for the visible light photocatalysts. The changes in the reactant and product concentrations with time are shown in Fig. S5 in the ESI.† The obtained reaction rates are listed in Table 4.
Entry | Conversion reaction rate (×10−3 mol L−1 s−1) |
---|---|
WO3 | 0.440 |
N–TiO2 | 0.298 |
N–Si–TiO2 | 0.214 |
V–N–Si–TiO2 | 0.160 |
From the product analysis and reaction rate analysis, the oxidation ability of WO3 was high, although the reaction was not selective. There was a discrepancy between the product analysis and reaction rate analysis for the oxidation abilities of N–TiO2 and N–Si–TiO2. This is probably because N–TiO2 lost its reactivity during the long reaction time, while the initial reaction rate was large during the reaction rate analysis carried out within a few minutes. Basically, it can be said that Si doping in TiO2 is effective for enhancing both the oxidation and reduction reactivities due to the decrease in the internal defects. But we could not confirm the enhancement of the reaction efficiency by vanadium deposition, because both the oxidation and reduction reactions were deactivated. This is probably because the deposition would reduce the number of active reaction sites.
![]() | (4) |
![]() | (5) |
r1 = kA[A]θV − k′AθA | (6) |
r2 = krθA | (7) |
![]() | (8) |
Footnote |
† Electronic supplementary information (ESI) available: Experimental setups are given in Fig. S1–S3. Examples of the fitting of the UV spectra using the reference spectra of the reactants and products are given in Fig. S4. See DOI: 10.1039/c3an02167j |
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