Lincheng Zhou*,
He Zhang,
Liqin Ji,
Yanming Shao and
Yanfeng Li
State Key Laboratory of Applied Organic Chemistry, College of Chemistry and Chemical Engineering, Institute of Biochemical Engineering & Environmental Technology, Lanzhou University, Lanzhou 730000, P. R. China. E-mail: zhoulc@lzu.edu.cn; Tel: +86-0931-8912528
First published on 28th May 2014
Tetrabromobisphenol A (TBBPA) is the most widely used brominated flame retardant around the world. In this study, we report that iron oxide decorated on a magnetic nanocomposite (Fe3O4/MWCNT) was used as a heterogeneous Fenton catalyst for the degradation of TBBPA in the presence of H2O2. Fe3O4/MWCNT was prepared by a simple solvothermal method, whereby an iron source (Fe(acac)3) and a reductant (n-octylamine) were allowed to react in n-octanol solvent. Monodisperse Fe3O4 nanoparticles of consistent shape were uniformly dispersed on the nanotubes. Samples were characterized by transmission electron microscopy, X-ray diffraction, Fourier transform infrared spectroscopy, X-ray photoelectron spectroscopy, Brunauer–Emmett–Teller surface area measurement, and vibrating sample magnetometry. The samples effectively catalyzed the generation of hydroxyl radicals (·OH) from H2O2, which degraded and subsequently mineralized the TBBPA. The whole process took four hours at near neutral pH. A degradation pathway for the system was proposed following analysis of intermediate products by gas chromatography-mass spectrometry. The quantification of Fe2+ and Fe3+ distribution before and after the recycling test of the composite were explored by X-ray photoelectron spectroscopy, in order to explain the stability and recyclability of the composite. Analysis of the results indicated that the magnetic nanocomposite is a potentially useful and environmentally compatible heterogeneous Fenton's reagent with promising applications related to pollution control.
000 tons,1 and China produces about 18
000 tons of the material per year. Despite its reactivity, TBBPA and its metabolites are released into the environment from either products treated with additives, or via reactions, and have been identified in samples of air, soil, and sediment,2 as well as in wastewater.3 Like most brominated aromatic flame retardants, TBBPA is lipophilic and difficult to degrade, and thus, adversely affects both environmental and biological systems.4 Therefore, the need to develop an effective method of clearing TBBPA from the environment is significant and urgent. Current methods for the removal of TBBPA from water include adsorption, biological degradation, ozonolysis, and catalytic oxidation.5–9 Because TBBPA can be broken into small, less toxic or harmless molecules, catalytic degradation is an increasingly important method of controlling this refractory organic pollutant. In 1894 Henry Fenton first reported that alcohols are oxidized in the presence of H2O2 and Fe(H2O)62+.10 The Fenton system is an attractive catalytic oxidation treatment for effective and exhaustive degradation because of its low cost, lack of toxic reagents (it employs Fe2+ and H2O2), circumvention of mass transfer limitations due to its homogeneous catalytic nature, and simplicity.11 However, homogeneous Fenton processes also present certain disadvantages, including a requirement for strong acidity (pH = 3.0), and the formation of a considerable amount of ferric hydroxide sludge during treatment, which requires further separation and disposal.12–15 Heterogeneous Fenton-like systems using Fe3O4 magnetic nanoparticles (MNPs) have been recently developed to overcome problems associated with homogeneous systems. The iron spinel Fe3O4 (magnetite) is known for high catalytic activity because it contains Fe2+, which is necessary for the initiation of the Fenton reaction, according to the classical Haber–Weiss mechanism. The octahedral configuration of ions in magnetite confers additional advantages as these sites can easily accommodate both Fe2+ or Fe3+, allowing the iron species to be reversibly oxidized and reduced without inducing structural changes.16 However, while Fe3O4 MNPs can be easily separated from the reaction medium under a magnetic field, they also tend to aggregate into larger clusters as a result of anisotropic dipolar attractions, which inhibits dispersibility and other properties.17,18
Carbon nanotubes (CNT) are a new class of small, adsorbent molecules that exhibit large specific surface areas, with hollow and layered structures. These CNT represent a class of adsorbents that are important for their potential ability to remove many kinds of organic compounds.19 Studies have demonstrated that CNT act as good supports for Fe3O4 MNPs, exhibiting high specific surface areas and low diffusion resistance. Studies have also reported the development of iron oxide/carbon nanostructures.20–23 For example, Deng et al.23 synthesized Fe3O4/MWCNT magnetic nanocomposites and used them as a Fenton-like catalyst to decompose acid orange II. These composites displayed higher activity (90% degradation) than Fe3O4 nanocomposites (38% degradation). However, the use of Fe3O4/MWCNT magnetic nanocomposites in a heterogeneous Fenton system to catalyze TBBPA degradation has not yet been reported.
In order to implement effective TBBPA degradation, we report in this work the preparation of Fe3O4/MWCNT using a simple solvo-thermal method. This new magnetic nanocomposite exhibits improved features, such as improved monodispersion and size control of the Fe3O4 nanoparticles on MWCNT, compared to our previous work.24,25 Moreover, this new Fe3O4/MWCNT exhibits high specific surface area and excellent stability, and can be used in a heterogeneous Fenton-like system for TBBPA degradation. Potential mechanisms of the degradation were proposed following analysis by gas chromatography-mass spectrometry (GC-MS).
:
2, 1
:
1 and 2
:
1.
The concentrations of TBBPA were analyzed by HPLC (LC-10AVP Plus, Shimadzu, Japan), equipped with a C-18 column under the following conditions: the mobile phase was an 80
:
20 (v/v) mixture of methanol and water; flow rate, 1.0 mL min−1; detection wavelength, 230 nm; column temperature, 30 °C; and retention time, 9.253 min.
Chemical analyses of the intermediates of TBBPA Fenton degradation were carried out using a GC-MS system (QP2010 Plus, Shimadzu, Japan) equipped with a fused silica capillary column (HP-5MS; length = 30 m; i.d. = 0.25 mm; film thickness = 0.25 μm). The column temperature was programmed as follows: 3 min at 80 °C; a temperature increase of 3 °C min−1 up to 300 °C; and 30 min at 300 °C. The helium gas flow rate was 1.0 mL min−1, and the sample size was 2 μL.
The residue rate of TBBPA (R, %) was calculated using eqn (1):
![]() | (1) |
:
2, 1
:
1, and 2
:
1 were observed by TEM under different magnifications (Fig. 1). Uniform, homogeneous, and non-agglomerated Fe3O4 MNPs were found decorated onto the surfaces of the MWCNT. Individual Fe3O4 MNPs or MWCNT were not observed, indicating that the preparation method was effective. The use of different ratios of Fe(acac)3 and MWCNT achieved different coverage densities of Fe3O4 on the MWCNT. The lowest iron content led to relatively low coverage density by small Fe3O4 particles (average diameter 4.19 nm; Fig. 1(a and b)). Increasing the iron content allowed for larger Fe3O4 particle growth, so the 1
:
1 Fe3O4/MWCNT sample exhibited 5.72 nm Fe3O4 particles (Fig. 1(c and d)), while a relatively high coverage density of 6.43 nm Fe3O4 particles was achieved in the sample with the highest iron content (Fig. 1(e and f)). The increasing Fe(acac)3 concentration resulted in higher concentrations of Fe3O4, which facilitated the thermodynamically stable growth of larger particles.
![]() | ||
Fig. 1 TEM images of 1 : 2 Fe3O4/MWCNT (a and b), 1 : 1 Fe3O4/MWCNT (c and d) and 2 : 1 Fe3O4/MWCNT (e and f). | ||
Fig. S1† shows the XRD patterns of both the pure Fe3O4 and the composite. The composite exhibited a different peak at 2θ = 25.78°, which can be indexed to the (002) reflection of the graphite structure of the MWCNT.28 The other peaks represent the pure Fe3O4 nanoparticles, as the signals at 30.05°, 35.12°, 43.50°, 54.14°, and 63.01°, are respectively consistent with standard data from the (220), (311), (400), (422), (511), and (440) reflections of the cubic spinel crystal structure of bulk magnetite (JCPDS file no. 19-0629).29 No obvious peaks from other phases were observed. The main Fe3O4 peaks appeared broadened, indicating a very small crystalline portion of the Fe3O4 MNPs. According to the full width at half maximum (FWHM) of (311) reflections, the average sizes of the Fe3O4 nanocrystalline particles from pure Fe3O4 and Fe3O4/MWCNT were calculated to be 5.7 nm and 5.9 nm based on the Debye–Scherrer formula, respectively. The almost similar crystallite of bare and decorated Fe3O4 suggests that MWCNT can be better support for the growth of metal oxide nanoparticles, without apparent agglomeration.
We observed a signal at 582 cm−1 in the FT-IR spectrum related to the Fe–O–Fe stretching vibration of Fe3O430 and a strong adsorption at 3438 cm−1 assigned to O–H stretching of multiwall CNT, which is consistent with previous research indicating a large number of carboxyl and hydroxyl groups on the surface of multiwall CNT (Fig. S2†).31 Results of the FT-IR indicated that the Fe3O4 MNPs were loaded successfully onto the MWCNT.
Samples were also analyzed by XPS (Fig. 2). The wide scan spectrum revealed photoelectron lines at binding energies of approximately 285, 528, and 711 eV (Fig. 2(a)), which were attributed to C 1s, O 1s, and Fe 2p orbitals, respectively. The O 1s spectrum indicates the presence of O 1s (528 eV) from the Fe3O4 (Fig. 2(b)).32 Fe 2p 1/2 and Fe 2p 3/2 peaks were observed at 710 and 725 eV (Fig. 2(c)), further confirming that the oxide in the sample was Fe3O4.33 The electron binding energy of C 1s at 285 eV was attributed to adsorbed carbon in the composites from the MWCNT (Fig. 2(d)).34
![]() | ||
Fig. 2 XPS spectra of 2 : 1 Fe3O4/MWCNT. (a) Wide scan, (b) O 1s spectrum, (c) Fe 2p spectrum, (d) C 1s spectrum. | ||
Nitrogen adsorption–desorption isotherms and pore size distributions were measured for all three samples and pure MWCNT (Fig. S3†). The BET method and Barrett–Joyner–Halenda (BJH) models were used to calculate specific surface area and porosity, respectively. The surface areas, pore volumes, and pore sizes of the different samples are summarized in Table 1. The specific surface area of pure MWCNT was 224 m2 g−1, and this value decreased with increasing iron content. The high specific surface areas shown by the magnetic CNT (145–174 m2 g−1) were greater than those of similar materials synthesized by other methods, which did not exceed 120 m2 g−1.35,36 Increases in specific surface area resulting from the present solvo-chemical route may be particularly beneficial to the adsorption and degradation of organic pollutants. This observed synergy is believed to result from the adsorptive properties of the support, which increase the rate of substrate degradation. Similar effects were reported by Hu et al.37 who determined that the degradation of pollutants, such as 17α-methyltestosterone, could be accelerated by their adsorption onto multi-walled carbon nanotubes.
| Sample | SBET (m2 g−1) | Pore volume (cm3 g−1) | Pore size (nm) |
|---|---|---|---|
2 : 1 Fe3O4/MWCNT |
145 | 0.6911 | 19.09 |
1 : 1 Fe3O4/MWCNT |
164 | 0.6570 | 16.07 |
1 : 2 Fe3O4/MWCNT |
174 | 0.6982 | 16.08 |
| MWCNT | 224 | 1.1771 | 26.07 |
The magnetic behaviors of the different Fe3O4/MWCNT samples and pure Fe3O4 exhibited typical S-type hysteresis loops with no residual magnetism or coercivity (Fig. 3), indicating that the nanoparticles were superparamagnetic. Saturation magnetization for three samples with increasing iron content increased by 6.91, 12.56, and 18.98 emu g−1, which was attributed to the strong magnetic properties of the Fe3O4. Although the composites exhibited lower saturation magnetization than pure Fe3O4 (73.29 emu g−1), they could still be easily separated from solution using an external magnetic field, which is a useful method for recycling biodegradable materials and reducing the cost of wastewater treatment.
Two kinds of mechanisms have been proposed to explain the strong oxidization associated with the Fenton reagent. The first mechanism involves the formation of high-valent iron–oxo intermediates, such as Fe
O2+, as reported by Bray and Gorin in 1932, and as illustrated by eqn (2) and (3) below:39
| Fe2+ + H2O2 → FeO2+ + H2O | (2) |
| FeO2+ + H2O2 → Fe2+ + H2O + O2 | (3) |
A related study by Churchill et al.40 reported the synthesis of a new molecular probe capable of detecting Fe3+ via fluorescence enhancement, which would allow for discrimination between Fe2+ and Fe3+ during the Fenton reaction. Results of that study confirmed the formation of a ferryl group (FeO2+) as an oxidative intermediate via DFT.
The second mechanism is the Haber–Weiss mechanism, which involves the generation of ·OH from H2O2 as a key step in the degradation process,41 as summarized in eqn (4) and (5).
| Fe2+ + H2O2 → Fe3+ + OH− + ·OH | (4) |
| Fe3+ + H2O2 → Fe2+ + H+ + ·OOH | (5) |
While no experimental methods are currently available to distinguish between these two kinds of mechanisms, we selected the latter method for our analysis. At low pH (<3.0) H2O2 can form a stable oxonium ion (H3O2+), which enhances the scavenging effect of the ·OH,42,43 and ·OH exhibits a higher oxidation capacity under acidic conditions, thereby inhibiting the decomposition of H2O2 into H2O and O2.44 Degradation is also poor under alkali conditions, as this affects the generation of ·OH, and produces hydroxide, which inhibits the catalytic ability of iron.45,46 Preliminary studies in our laboratory indicated that optimal degradation occurred at pH 5.0, and this pH was maintained for all subsequent degradation experiments.
| ·OH + H2O2 → HO2· + H2O | (6) |
| ·OH + HO2· → O2 + H2O | (7) |
| ·OH + ·OH → H2O2 | (8) |
All TBBPA degradation experiments were subsequently conducted using 27 mmol L−1 H2O2, as this concentration produced the highest degradation.
:
1 Fe3O4/MWCNT catalyst (Fig. S6†). TBBPA residue rates dropped from 96.3 to 3.2% as the concentration of the composite increased from 0.0 to 4.0 g L−1. This was due to the increased number of active sites on the oxide surface, which accelerated the decomposition of H2O2 and the dissolution of iron to produce more ·OH.37,50 A sharp decrease in TBBPA degradation was observed when the concentration of 2
:
1 Fe3O4/MWCNT was lower than 0.5 g L−1, while only slight changes were observed when the concentration of 2
:
1 Fe3O4/MWCNT exceeded 0.5 g L−1. However, at 0.5 g L−1, TBBPA could be removed almost completely, so 0.5 g L−1 of 2
:
1 Fe3O4/MWCNT was used in subsequent experiments.
:
2, 1
:
1, and 2
:
1), and their abilities to degrade TBBPA were compared (Fig. 4). Improved degradation was observed with increasing iron content, as the three samples exhibited decreasing residue rates of 23.26, 11.13, and 4.65%, respectively. The increased activity of the composites, resulting from increased iron content, was attributed to an increase in the number of active sites, which are visible in the TEM (Fig. 1). This reaction was considered a pseudo-first-order reaction, with the concentration Ct of TBBPA at reaction time t being described as follows:51
Ct = C0 exp(−kt)
| (9) |
:
1 Fe3O4/MWCNT and Fe3O4 were evaluated under optimal conditions. In order to differentiate between degradation and adsorption, adsorption tests were also conducted using the three kinds of materials (2
:
1 Fe3O4/MWCNT, pure Fe3O4 and pure MWCNT). As seen in Fig. 5, the adsorption of TBBPA was almost negligible in the presence of pure Fe3O4, which might have been due to its low surface areas. The increased surfaces areas of both 2
:
1 Fe3O4/MWCNT and pure MWCNT resulted in predictable increases in adsorption performance, with TBBPA residual rates of 52.34 and 33.55%, respectively. However, when H2O2 was added, The TBBPA residual rate for 2
:
1 Fe3O4/MWCNT dropped to 4.87%, while the TBBPA rate when pure Fe3O4 was used as a catalyst for TBBPA degradation was 60.56%. These comparisons were made based on equal weights of the catalysts. Results of these experiments indicated that the degradation efficiency of 2
:
1 Fe3O4/MWCNT was two times higher than that of Fe3O4, and that approximately twice as much TBBPA was degraded as adsorbed. This significant activity enhancement can be attributed to homogeneous dispersion of the Fe3O4 nanoparticles, which appears to increase the number of active sites for substrate access.
:
1 Fe3O4/MWCNT and pure Fe3O4 were evaluated via their successive use in TBBPA degradation (Fig. 6). After 10 cycles, the TBBPA residual rate remained at 6.8% (Fig. 6(a)), and the saturation magnetization of composite after 10 cycles was 16.93 emu g−1 (Fig. 6(b)), which represented only a 1.1% decrease from its original value. By contrast, the saturation magnetization of pure Fe3O4 after 10 cycles was 61.69 emu g−1 (Fig. 6(b)), which represented a 15.8% decrease from its original value. To further demonstrate the stability of the structures, XPS was used to analyze the catalysts before and after the Fenton reaction. The details of the Fe 2p peaks (Fe 2p 1/2 and Fe 2p 3/2) of the 2
:
1 Fe3O4/MWCNT and pure Fe3O4 before and after their use during TBBPA degradation are presented in Fig. 6(c–f) and Table S1.† The Fe 2p 1/2 peak for Fe3O4 was deconvoluted into the Fe3+ and Fe2+ peaks. Before use, the corresponding binding energy values were 712.00 eV and 711.00 eV, respectively (Fig. 6(c)), and these values did not change significantly after 10 cycles of use for TBBPA degradation (711.80 eV and 710.90 eV: Fig. 6(d)). Calculation of the peak areas indicated that 67.6% of the total iron surface atoms were Fe3+, while 32.4% were in the Fe2+ state, which was consistent with the Fe3O4 crystal structure. For samples evaluated after 10 cycles of TBBPA degradation, the concentration of Fe3+ on the surface increased to 70.0%, while Fe2+ decreased to 30.0%, which indicated that some of the Fe2+ on the outermost layer of the catalyst was oxidized into Fe3+ during the Fenton reaction. Meanwhile, we used the same methods to analyze the pure Fe3O4. Before use, the corresponding binding energy values were 711.91 eV and 710.62 eV, respectively (Fig. 6(e)). After 10 cycles of use for TBBPA degradation, these values were 712.20 eV and 711.05 eV (Fig. 6(f)). Fe2+ surface concentration was 32.7% in the pure Fe3O4 before use, but only 27.8% after use. It is well known that the oxidation of the ferrous iron by H2O2 is much faster than the reduction of the ferric iron by H2O2. Thus, in order to speed up the redox cycle between ferrous and ferric species, it should improve the reduction of the ferric iron by H2O2.23 Obviously, the reduction of the ferric iron in the Fenton system use Fe3O4/MWCNT was more efficient than use pure Fe3O4. Collectively, these results suggested excellent stability and durability of the composite.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra02333a |
| This journal is © The Royal Society of Chemistry 2014 |