Zi-Yian Limab,
Chunzheng Wua,
Wei Guo Wanga,
Kwang-Leong Choy*c and
Hongfeng Yin*a
aNingbo Institute of Material Technology and Engineering, 519 Zhuangshi Road, Zhenhai District, Ningbo 315201, China. E-mail: yinhf@nimte.ac.cn
bUniversity of Nottingham, Ningbo China, 199 Taikang East Road, University Park, Ningbo 315100, China. E-mail: zx08427@nottingham.edu.cn
cUCL Institute for Materials Discovery, University College London, Kathleen Lonsdale Building, Gower Place, London, WC1E6BT, UK. E-mail: k.choy@ucl.ac.uk; Tel: +44 (0)207679 3855
First published on 13th July 2015
Steam reforming of methane is a versatile technology for hydrogen production in oil refinery and fuel cell applications. Using natural gas is a promising method to produce rich-hydrogen gas. Ni@yolk–ZrO2 catalyst is used to study steam reforming of methane under various GHSVs, steam-to-carbon (S/C) ratio, and its recyclability. The catalyst was characterized using a combination of XRD, TEM, AAS, TPR, TPH, TGA, BET, XPS, and Raman techniques. The catalyst is evaluated on time stream and identify its anti-agglomeration property and coking mechanism. From the characterization of TEM and XPS establish the information of Ni particles mobility in the catalyst, which active metal particle size was controlled under the yolk–shell structure framework. Furthermore, the results from TGA, TPH, and Raman analysis of the used Ni@yolk–ZrO2 catalyst showed the characteristic of inhibiting formation of highly ordered carbon structure.
Several studies discuss enhancing the stability of Ni-based catalyst for the reforming reaction. Promotes such as alkaline earth (MgO or CaO) are often used to lower the coke formation and provide higher stability against sintering.9 However, the addition of these promoters obstructs the reduction of NiO leading to less active metals involve in the reactions. It has been observed that promotion with K or Ca increases the formations of NiAl2O4 phase, whereby Ni was substituted in the inert spinel structure and became inactive.10 It was reported that adding tolerable alkaline metal oxide suppressed the coke deposition in the reforming reaction. Hence, it is crucial that the modification of Ni-based catalysts do not compromise the activity.
It is evident that the reducible support (e.g. CeO2) provides better stability and coke resistance in comparison with non-reducible supports.11,12 As they have direct advantage of oxygen storage capacity that significantly reduce the coke formation on the catalyst surface.13 Ceria and ceria-doped supports are well known for their reversible exchange of lattice oxygen during reaction.14 However, CeO2 support is vulnerable to sintering and loses its oxygen storage capacity (OSC) at high temperatures (e.g. above 500 °C).15 Also, CeO2 could fully cover the active metal during the redox reactions due to their amorphous feature which lead to deactivation.16
The activity of the catalyst often depends on the size and extent of metal dispersion.17,18 Small particles increase metal dispersion and also provide more active site (steps/kinks) on the surface.19 The energy barrier for methane dissociation is much lower at step sites. Therefore, the rate of reaction increases with smaller particles as they consisted of highly concentrated active phase of step sites.20 Besides, small particles below a critical size have also been reported to be more resistant to coke formation.21 The highly dispersed active metal particles also tend to minimize surface energy by strongly interact with the support and reduce sintering occurrence. Hence, Ni with good particle size homogeneity and metal support interaction are essential for a highly stable catalyst.
The preparation method often influences the structure and morphology of the catalyst. Recently, a method of embedding the active metal nanoparticles in inorganic cavities shows promising application in preventing sintering of active metal.22 Among these materials, highly defined nanostructure of core–shell and yolk–shell structure have demonstrated excellent properties in various applications, for example, Au–Ni@SiO2 for hydrolytic dehydrogenation of ammonia borane,23 metal@TiO2 yolk–shell nanostructures for photocatalytic dye degradation24 and Au@ZrO2 for CO oxidation.25 Of particular interest is Au@ZrO2 yolk–shell nanostructure. This is because it has great potential to be developed for highly stable and ease of gaseous exchange in catalytic applications. In addition, the structure is easy to be modified such as its porosity through modification of the shell to further improve its catalytic performance.26 In this paper, we report a Ni@yolk–ZrO2 catalyst synthesized via double template emulsion method which shows substantial long term high activity and successfully performed for multiple cycles without deterioration under operation mode of steam reforming of methane at S/C molar ratio of 2.5 (Fig. 1).
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Fig. 1 A schematic diagram of the synthetic route of Ni@yolk–ZrO2 catalyst, and the associated TEM of the structures and core size distributions. |
X-ray diffraction patterns were recorded using Bruker D8 Advance with Cu-Kα radiation (λ = 1.5418 Å) in the 2θ range of 10–90°. Transmission electron microscopy (TEM), model JEM 2100 was used to study the morphology and microstructure of the catalyst. The TEM specimens were prepared by dropping a trace amount of the sample dispersed in ethanol on a carbon coated copper grid (300 mesh). The BET surface area measurement was carried out using a Micrometrics ASAP 2020M apparatus at 77 K. Prior to the measurement, the sample was degassed at 300 °C for 5 h under vacuum. Temperature-programmed reduction (FINESORB3010E, Zhejiang Fintec Co.) was performed to determine the nickel species and its reducibility for each catalyst. Typically, catalyst was filled into a U-shape quartz tube and held by quartz wool. Prior to reduction, the sample was treated with pure Ar for 30 min at 300 °C to remove any impurities. The temperature was then cooled down to room temperature. 10%H2/Ar (25 ml min−1) was introduced, and the temperature was increased from room temperature to 800 °C with a heating rate of 5 °C min−1. A temperature programmed hydrogenation was used to identify the carbon species of the used catalyst. Typically, used catalyst (30 mg) was loaded into a U-shape quartz tube and held by a quartz wool. Prior to hydrogenation, the sample was treated under pure Ar for 3 h at 100 °C and cooled down to room temperature. Then, a mixture of 10%H2/Ar (25 ml min−1) was introduced into the sample. After 2 hours, the temperature was increased to 900 °C with a heating rate of 5 °C min−1. X-ray photoelectron spectroscopy (XPS) spectra were recorded on a Shimadzu Axis Ultradld spectroscope (Japan) using the monochromatized Al Kα radiation resource at room temperature and under a vacuum of 10−7 Pa (10−9 Torr). The starting angel of the photoelectron was set at 90°. The spectrum was calibrated with a C 1s spectrum of 248.8 eV. Raman spectra were collected using a Renishaw inVia Reflex (λ = 532 nm) and a CCD detector. The spectrum acquisition consisted of 10 accumulations for 30 s. The spectra were recorded at ambient temperature. Thermogravimetric analysis (TGA) was conducted using Perkin-Elmer Pyris Diamond TGA equipment. The used catalysts were preheated under a flow of nitrogen (100 ml min−1) for 30 min. Then the samples were heated in air (100 ml min−1) by raising the temperature from room temperature to 1000 °C at a rate of 10 °C min−1.
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Fig. 3 TEM images of Ni@yolk–ZrO2 before (a) and after 48 h (c) steam reforming test and their Ni core particle size distribution (b) and (d) respectively. |
The TEM micrographs of Ni@yolk–ZrO2 catalyst before and after steam reforming test are shown in Fig. 3 and 5. Before reforming test, the Ni particles are uniformly distributed over the ZrO2 hollow shell and no apparent aggregation of particles was observed. The average particle size of Ni is about 8.9 nm. After 48 h on steam reforming of methane, the particle size increased to circa. 9.6 nm. The crystallite size of Ni and the average Ni particle size from TEM observation was 8.9 nm. Fig. 4 shows the XPS Ni 2p peak of freshly reduced Ni@yolk–ZrO2 with detectable Ni particles over the catalyst surface, in contrast, the used-catalyst showed almost the non-existence of Ni particles over the catalyst surface. From the XPS depth analysis,29,30 Ni particles have been detected partly in the matrix of ZrO2 hollow shell before testing and inside the hollow shell after steam reforming of methane testing. In addition, the Ni mass concentration (Table 1) is diminished after the reforming testing of Ni@yolk–ZrO2 catalyst while the impregnated Ni/ZrO2 remained the same. This result indicated Ni particles have been moving toward inside the ZrO2 hollow shell during catalytic testing.
Catalysts | Ni 2p (%) | O 1s (%) | Zr 3d (%) | Si 2p (%) |
---|---|---|---|---|
Ni@yolk–ZrO2-before | 2.78 | 36.3 | 45.5 | 15.41 |
Ni@yolk–ZrO2-after | 0 | 31.13 | 40.02 | 22.69 |
Ni/ZrO2-before | 7.88 | 21.57 | 70.54 | — |
Ni/ZrO2-after | 7.49 | 36.13 | 56.38 | — |
The BET isotherm graph (Fig. 6) showed Ni@yolk–ZrO2 has Type-IV isotherm characteristic and hysteresis loop of category H3. It has high amount micropore (P/Po < 0.1) as compared to impregnated Ni/ZrO2. It also has the characteristic of multilayer adsorption before the onset of capillary condensation. The slope of the multilayer adsorption suggesting slit-shaped pore might present between the nano-size ZrO2 grains in the shell which would allow gaseous exchange to occur during reactions. XRD patterns of Ni@yolk–ZrO2 showed broadening peaks of tetragonal phase of ZrO2, implicating the occurrence of multilayer adsorption of the shell is indeed promoting the high degree of reactants and products exchange. Besides, the capillary condensation is the void space between the Ni core and ZrO2 shell with 18 nm pore. The void space would allow active Ni particle to move freely around but was inhibited to move outside the shell attributed to the presence of the slit-shaped framework of the ZrO2 shell. Such characteristic is advantageous to significantly reduce active Ni particles from agglomerating with each other and limiting their particle growth.
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Fig. 6 BET isotherm of Ni@yolk–ZrO2 (a) and Ni/ZrO2 (b). Inset: pore size distribution of Ni@yolk–ZrO2 (c) and Ni/ZrO2 (d). |
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Fig. 7 Catalytic steam reforming of methane on Ni@yolk–ZrO2 and Ni/ZrO2 catalyst (a). Catalytic performance and H2/CO ratio under various GHSVs and S/C ratio on Ni@yolk–ZrO2 catalyst (b). |
Analysing the effect of the reaction temperature on the catalytic performance of Ni@yolk–ZrO2, a temperature of 750 °C was kept to study the effect of GHSVs. The purpose of this study is to optimize the possibility of reactants that could be process into synthesis gas. Moreover, steam reforming is an energy consuming process and it is necessary to reduce the process cost. Hence, the methane content in the feed was changed, and the results are depicted in Fig. 7b. As the GHSVs increased, the methane conversion decreased for all S/C conditions. The catalyst performance maintained up to 85% or above of methane conversion (for S/C = 1.5 and S/C = 2), when S/C = 1, the methane conversion was maintained up to 70% or above. Also, it can be observed that the H2/CO ratio for all conditions is particularly low at GHSV of 20000 ml gcat−1 h−1 and a higher content of CO was produced at this operating condition.
The same catalyst was subjected to recyclability test of steam reforming of methane under S/C = 2.5. The catalyst was tested for 4 hours, oxidizes in air at 500 °C for 1 hour, reduced at the same temperature for 1 hour, and repeated these cycles for 5 times. The catalyst exhibited a methane conversion of 90% which is almost constant along 5 reaction cycles (Fig. 9a). Also, the catalyst was tested on stream and remained active and continuously producing synthetic gas for 150 hours (Fig. 9b). It is remarkable that the catalyst performance of the Ni@yolk–ZrO2 exhibiting superior catalytic effect in steam reforming of methane.
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Fig. 9 Reusability of Ni@yolk–ZrO2 on steam reforming of methane (a) and 150 hours durability test on Ni@yolk–ZrO2 catalyst (b). |
2CO → CO2 + C | (3) |
CH4 → 2H2 + C | (4) |
Eqn (3) and (4) were the Boudouard reaction and methane decomposition which were preliminary formation of carbon nanotubes and graphites.32 Therefore, it is essential to determine the carbon species formed in the Ni@yolk–ZrO2 catalyst as compared to impregnated Ni/ZrO2. Fig. 10a represents the TGA of both tested catalyst. It is noticed that Ni@yolk–ZrO2 has higher weight loss than Ni/ZrO2 with carbon deposition rate of 1.15 mgc gcat−1 h−1 after 48 hours. This might be due to methane dissociation33 is higher for smaller Ni particles size of Ni@yolk–ZrO2 than Ni/ZrO2; hence a higher weight loss would occur on the Ni@yolk–ZrO2 catalyst. In order to understand the carbon species formed in the catalysts, it was subjected to TPH after steam reforming of methane. As identified in Fig. 10b that the surface carbon species on Ni@yolk–ZrO2 is weak than Ni/ZrO2 and the first peaks of carbon species are at 260 °C and 293 °C respectively. The first peak might be amorphous carbon (α-carbon) on the nickel sites. Second and third peaks would be whisker carbon (β-carbon) or graphitic carbon (γ-carbon) exists in the catalyst. It can be seen that Ni/ZrO2 has a broad shoulder peak at 360 °C and a small peak at 835 °C. The impregnated Ni/ZrO2 catalyst has higher order carbon species formed during the steam reforming of methane as compared to Ni@yolk–ZrO2 with only α and β carbon. The main carbon deposited in Ni@yolk–ZrO2 was amorphous carbon due to high density of kinks existing in small Ni particles size and this amorphous carbon was readily to be reacted with steam. Furthermore, both of the catalyst were carried out under S/C = 1 with the same GHSV of 50400 ml gcat−1 h−1 for 12 h in order to understand the carbon species formation in Ni@yolk–ZrO2. From Fig. 11, the weight loss is significantly higher with 5% carbon (3.29 mgc gcat−1 h−1) was deposited. However, from the TPH analysis, the first peak diminished and second peak was intensified. As for the third peak which occurred at 650 °C indicating a higher ordered carbon has formed, but the temperature lies lower than impregnated Ni/ZrO2 catalyst. This phenomenon suggesting yolk–shell structure inhibiting the formation of highly ordered carbon in Ni@yolk–ZrO2 catalyst. Further validation of Raman (Fig. 12) of the tested catalysts (S/C = 2.5 and S/C = 1) showed the presence of the spectra of D band and G band of carbon has the relative intensity ratio ID/IG of 0.94 and 0.96. It demonstrates the ZrO2 shell has inhibited the continuous growth of whisker carbon or graphitic carbon from Ni particle. It can be concluded that Ni@yolk–ZrO2 exhibiting the capability of inhibiting the formation of higher ordered carbon during steam reforming of methane.
Catalyst | Ni (wt%) | GHSV (ml gcat−1 h−1) | Conditions | Temperature (°C) | XCH4 |
---|---|---|---|---|---|
Ni@yolk–ZrO2 | 5.08 | 50![]() |
SRM (S/C = 2.5) | 750 | 93.0 |
Ni@SiO2 yolk–shell3 | 89 | 100![]() |
SRM (S/C = 4) | 700 | 90.0 |
10 wt% Ni/MgAl2O4 (ref. 4) | 10 | 54![]() |
SRM (S/C = 2) | 750 | 97.2 |
NiO-350@meso-SiO2 | 54.8 | 72![]() |
POM | 750 | 93.0 |
Ni–yolk@Ni@SiO2 (ref. 6) | 18.6 | 36![]() |
DRM | 800 | 90.0 |
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