Takeshi
Konya
a,
Tomokazu
Katou
a,
Toru
Murayama
a,
Satoshi
Ishikawa
a,
Masahiro
Sadakane
b,
Douglas
Buttrey
c and
Wataru
Ueda
*a
aCatalysis Research Center, Hokkaido University, N-21, W-10, Sapporo 001-0021, Japan. E-mail: ueda@cat.hokudai.ac.jp; Fax: +81 11 706 9163; Tel: +81 11 706 9164
bChemistry and Chemical Engineering, Department of Engineering, Hiroshima University, 1-4-1 Kagamiyama, Higashi-Hiroshima 739-8527, Japan. E-mail: sadakane09@hiroshima-u.ac.jp; Fax: +81 82 424 5494; Tel: +81 82 424 4456
cCenter for Catalytic Science and Technology, Department of Chemical Engineering, University of Delaware, Newark, DE 19716, USA. E-mail: dbuttre@udel.edu; Fax: +1 302 831 1048; Tel: +1 302 831 2034
First published on 30th August 2012
Four distinct structural types (orthorhombic, trigonal, tetragonal and amorphous) of Mo3VOx catalyst were each synthesized by a hydrothermal method as a single phase, characterized structurally and tested for oxidative dehydrogenation of ethane. A common structural feature of the catalysts is that the materials are a layer-type structure and constructed with pentagonal {Mo6O21} units. The arrangement of the pentagonal units can form heptagonal channels to create different structural features. The orthorhombic Mo3VOx catalyst has microporosity due to the open heptagonal channels adsorbing nitrogen molecules and showed the highest activity for the reaction among four distinct catalysts. Furthermore, this phase appeared to be most active, currently, compared to other complex metal oxide catalysts reported. An observed positive relation between the microporosity and the oxidation activity suggests that the catalytic oxidation takes place at the heptagonal channels.
The catalysts in the first category are, for example, MgO-based mixed oxides,4,5 rare earth metal oxides,6,7 and oxyhalides8,9 particularly oxychlorides.1 These catalysts tend to show very high selectivity to ethene at high ethane conversion because the catalysts themselves do not have high intrinsic catalytic oxidation ability, which is the reason why the catalyst needs high reaction temperatures. The second catalysts, representatively Ni–Nb–O,10 have recently emerged and their catalytic activity apparently depends on the nature and state of group 8 elements11 since simple oxides of group 8 elements are usually very active for ethane oxidation but non-selective.
The catalysts in the third category also have a wide variety of oxide catalyst systems but in many cases contain V as a key element.3 In this category the Mo–V–O complex oxide system has been recognized as the most promising for application.12 This catalyst has interesting and long history of development, which dates back to the report by Thorsteinson in 1978.13 They found that Mo–V–O showed high ethane oxidation activity even at temperatures lower than 300 °C only when the catalysts gave an XRD peak at 22° (Cu Kα). They also found that Nb was the most effective additive element. Since this report, there has been, however, no appreciable progress in this catalyst system for ethane oxidation. Meanwhile catalysts in which Te or Sb was added to Mo–V–Nb–O have been developed by Mitsubishi Chemicals for propane ammoxidation.14 The catalyst also gave an XRD peak at 22° (Cu Kα) and more importantly is a crystalline material formed, so-called M1 structure, which is iso-structural of orthorhombic Mo3VOx materials dealt with in the present study. After this discovery much attention has been paid to this catalyst system not only for propane oxidation but also for ethane oxidation. Eventually Mo–V–Te–Nb–O was found to show 87% conversion of ethane with 84% selectivity to ethene at 400 °C15 and Mo–V–Sb–O also showed similar catalytic performance.16 Presently, there is no doubt that the catalytic materials found by Thorsteinson are of Mo–V–Te–Nb–O type. The main concern still remaining about this catalytic system is whether Te, Sb, and Nb are necessary elements in the course of ethane oxidation or not. We have recently succeeded in synthesizing a well-crystallized, single phasic orthorhombic Mo3VOx17–20 and found that this catalyst showed extremely high activity for the oxidative dehydrogenation of ethane, which is better than that of the Mo–V–Te–Nb–O catalysts. This result clearly indicates that the elements other than Mo and V are not essential but the structure formation is more important.
Here in this report we investigate the genesis of such high oxidation activity of the orthorhombic Mo3VOx catalyst by comparing four distinct types of Mo3VOx catalyst with different crystal structures.
Elemental compositions were determined by an inductive coupling plasma (ICP-AES) method (ICPE-9000, Shimadzu). XRD patterns were measured by using an X-ray diffractometer (RINT-Ultima III, Rigaku) with Cu Kα (tube voltage: 40 kV, tube current: 20 mA). Unit cell parameters were refined using the Rietveld program with Materials Studio 5.5.3 (Accelrys). SEM images were taken using an electron microscope (JSM-6360LA, JEOL) and aberration-corrected high-angle annular dark-field (HAADF) STEM operated at an accelerating voltage of 200 kV was used to image the materials with a JEOL 2100F equipped with a Corrected Electron Optical Systems GmBH spherical aberration corrector on the illumination system.23,24 Since the trigonal sample used for the HAADF-STEM analysis was not highly crystallized and various crystal faults and disordered regions were observed in the images, we took an image of the disordered part as for the amorphous sample23 and the image is shown in Fig. 4.
FT-IR spectra were obtained using a spectrometer (Paragon 1000, Perkin Elmer) at room temperature in the range of 500–1100 cm−1. Raman spectra were obtained using a spectrometer (in Via Reflex, Renishaw, 2 cm−1 spectral resolution) under the conditions of 532 nm wavelength and 30 s collection time. N2 adsorption isotherms at liq. N2 temperature were obtained using an auto-adsorption system (BELSORP MAX, Nippon BELL). Surface areas and micropore volumes were determined using a t-plot. Prior to N2 adsorption, the catalysts were evacuated under vacuum at 300 °C for 2 h.
Fig. 1 SEM images of orthorhombic (a), trigonal (b), amorphous (c), and tetragonal (d) Mo3VOx. |
Catalyst | Main preparatory conditiona | Average rod | Chemical compositionc | Lattice parameter/nm | ||
---|---|---|---|---|---|---|
diameterb/μm | a | b | c | |||
a For more details, see the Experimental section. b Average of 30–200 crystalline in SEM images. c Determined by ICP-AES. | ||||||
Orthorhombic Mo3VOx | pH = 3.2 | 0.42 | Mo3.00V0.97Ox | 2.1083 | 2.6569.5 | 0.3997 |
Trigonal Mo3VOx | pH = 2.2, Mo compound | 0.22 | Mo3.00V0.97Ox | 2.1380 | 2.1380.9 | 0.3994 |
Amorphous Mo3VOx | High concentration | 0.39 | Mo3.00V1.15Ox | — | — | 0.3996 |
Tetragonal Mo3VOx | Heat-treatment | 0.82 | Mo3.00V1.15Ox | 2.2847 | 2.2847 | 0.3958 |
Fig. 2 shows XRD patterns of four catalysts, calcined and used for the catalytic reaction. Two diffraction peaks at 22° and 45° were commonly observed for all the samples, indicating that the materials are all of a layered-type structure with the same layer lattice distance of about 0.4 nm. Since the SEM image showed the same crystal shape (Fig. 1), crystal growth by layer stacking took place in the direction parallel to the rod, giving two clear common diffraction peaks which can correspond to 001 and 002 reflections by taking the c-axis parallel to the rod. From these peaks, c lattice parameters were calculated and are listed in Table 1. As expected, four samples have almost similar values at around 0.399 nm.
Fig. 2 XPD patterns of orthorhombic (a), trigonal (b), amorphous (c), and tetragonal (d) Mo3VOx catalysts heat-treated (lower) and used for catalysis (upper). |
Characteristic diffraction peaks depending on the catalysts were observed at the low angle region less than 10°. The appearance of the peaks indicates crystals with large a and b lattice parameters which were calculated by Rietveld refinement and are listed in Table 1 except for the amorphous Mo3VOx. The amorphous Mo3VOx gave only a very broad peak at the low angle region, which obviously indicates that the material is not fully crystallized. Since the SEM image (Fig. 1(c)) shows uniform rod-shaped materials, the rod materials appear to be crystallized in the c-direction along the rod but are not orderly crystallized both in a- and b-directions, which can satisfy the observed XRD diffraction in Fig. 2c.
All the samples were found to be stable by XRD after the catalytic test, although slight changes in peak positions and in relative peak intensities were observed, particularly those at the low angle region. We have reported that the lattice parameters depend on the reduced state of the samples.22 On the other hand, we consider that the change of the relative peak intensity is due to a structural deformation and therefore, further investigation on this phenomenon is now underway.
Structure similarities among four materials were further exemplified by elemental analysis, FT-IR and Raman spectroscopy. Chemical compositions were determined by ICP-AES after dissolution of the samples in aqueous ammonia solution and the results are listed in Table 1. The compositions of the orthorhombic, trigonal, amorphous and tetragonal materials were determined to be Mo3.00V0.97Ox, Mo3.00V0.97Ox, Mo3.00V1.15Ox and Mo3.00V1.15Ox, respectively. The amorphous and tetragonal materials are obviously V-rich. Although the reason is unclear at the present stage, excess accommodation of V in the lattice of the amorphous material and some loss of Mo during the phase transformation of the orthorhombic material seem to be possible reactions. Nevertheless, it appears that the chemical composition among four materials is not dissimilar.
FT-IR and Raman spectroscopic investigation provides more atomic level information. The obtained spectra are summarized in Fig. 3. In FT-IR spectra, bands at 915 cm−1 ascribable to VO, 870 cm−1 for MoO, 817, 716 and 652 cm−1 for Mo–O–Mo and 604 cm−1 for V–O–Mo were observed for all the samples and additional bands at 789 and 572 cm−1 were observed only for the tetragonal sample. Similarly, in Raman spectra, the main band at 870 cm−1 was observed for all the samples. Furthermore, this main band was associated with a few bands in the cases of the orthorhombic, trigonal and amorphous samples but less in the case of the tetragonal sample. As Raman bands similar to these main bands were observed for polyoxometalates like {[K10Mo72V30O282(H2O)56(SO4)12]26−}25,26, {[Mo132O372(H2O)72(CH3CO2)30]42−}27 and {[H3Mo57V6(NO)6O183(H2O)18]21−}28 all of which were constructed by a linkage of the pentagonal {Mo6O21} building units, the Raman bands observed for the Mo3VOx materials clearly exhibit the presence of the pentagonal {Mo6O21} units in each lattice, which is also a common structural feature of all the samples. However, the tetragonal material appears to contain different metal–oxygen bonds because the FT-IR and the Raman spectra of the tetragonal material were different from the others. Conversely, it is notable that the FT-IR and the Raman spectra are comparable among the orthorhombic, trigonal and amorphous samples, revealing that the structural features of the amorphous material are close to that of the orthorhombic sample, but with disordered pentagonal {Mo6O21} units arranged in the a- and b-directions.29 In other words, the amorphous phase is not like the tetragonal phase, which is an important conclusion as for many years the amorphous phase has been considered to be similar to the tetragonal phase in the study of acrolein oxidation to acrylic acid.30
Fig. 3 FT-IR (A) and Raman (B) spectra of orthorhombic (a), trigonal (b), amorphous (c), and tetragonal (d) Mo3VOx catalysts. |
All the above structural characterizations were fully confirmed by HAADF-STEM images23,24 shown in Fig. 4 along with structure models for the four samples. The first clear point from the images is that the pentagonal {Mo6O21} units are visible in the a–b plane of all the materials and arranged in different manners forming different pentagonal unit network structures. The second point is that the image contrast of the pentagonal {Mo6O21} unit parts is brightest compared to that of the other structural parts, which strongly supports that the pentagonal unit is constructed with Mo only and the other octahedra in the structures contain V as well as Mo. The third point, which seems to be most important, is that in the images in Fig. 4(a), (b) and (d) two dark spots with different sizes, large and small, are visible and correspond to two structural units; the heptagonal channel and the hexagonal channel, respectively. In the tetragonal material, the dark spot due to the heptagonal channel was not observed. The final point is that the contrast at the heptagonal channel was dark, meaning that there are no elements present and the channel is empty. This observation is related to microporosity of the materials that will be described in the next section.
Fig. 4 Structures model (left) and HAADF-STEM images (right) of orthorhombic (a), trigonal (b), amorphous (c), and tetragonal (d) Mo3VOx. |
By referring to the structural models shown in Fig. 4, the structural information obtained can be summarized as follows:
(1) All four Mo3VOx materials possessing similar chemical compositions assume the same layer-type structure in the c-direction and form a long-rod shaped crystal.
(2) All four Mo3VOx materials contain the same building units, pentagonal {Mo6O21} units.
(3) The overall crystal structure is determined by the network arrangement of the pentagonal {Mo6O21} units in the a–b plane.
(4) The orthorhombic, trigonal and amorphous Mo3VOx are classified into similar structure-type groups but the tetragonal Mo3VOx is excluded because the former materials contain the empty heptagonal channels but the latter does not.
Here we measured microporosity of four distinct Mo3VOx materials for comparison and the results are illustrated in Fig. 5. By using N2 adsorption isotherms, micropore volume and external surface area were calculated from the t-plot (Table 2). As can be seen in Fig. 5, the trigonal phase also showed N2 adsorption at low relative pressure as the orthorhombic material did. It is apparent that the trigonal material has microporosity, which is natural because of the structure. However, the adsorption capacity was determined to be low compared to that of the orthorhombic material as listed in Table 2. From the structural point of view, both the materials should show a similar micropore volume per gram. The observed difference presumably results from partial occupation of the heptagonal channel of the trigonal material by additionally accommodated octahedra. This consideration is partly supported by the fact that the site occupancy at three-membered octahedral sites in the middle of three heptagonal channels is low, as evidently shown by dark contrast at this site in the HAADF-STEM images (Fig. 4b). This result indicates that the three membered-octahedra in this site cannot be stably accommodated and suggests that additional octahedra may exist in heptagonal channels to stabilize near three-membered octahedra. In fact we observed additional octahedra in the heptagonal channels by HAADF-STEM analysis.23
Fig. 5 Nitrogen adsorption isotherm ((A) normal P/P0 range, (B) low pressure P/P0 range) of orthorhombic (a), trigonal (b), amorphous (c), and tetragonal (d) Mo3VOx. |
Catalyst | Micropore | External surface areab/m2 g−1 | Conversionc/% | Selectivityc/% | Activation energyd | |||
---|---|---|---|---|---|---|---|---|
Volumea/10−3 cm3 g−1 | C2H6 | O2 | C2H4 | COx | CH3COOH | kJ mol−1 | ||
a Measured by N2 adsorption at liq. N2 temperature and determined by the t-plot. b External surface areas were also determined by the t-plot. c Data at ca. 335 °C under the reaction condition described in the Experimental section. d Activation energy for ethane oxidation. e Catalytic data were collected with a reduced amount of the catalyst (0.1 g). | ||||||||
Orthorhombic Mo3VOx | 14.0 | 8.2 | 56.0 | 64.8 | 81.8 | 13.5 | 4.7 | 82.1 |
Orthorhombic Mo3VOxe | — | — | 20.0 | 14.3 | 94.3 | 3.5 | 2.2 | — |
Trigonal Mo3VOx | 4.0 | 12.4 | 19.6 | 19.3 | 82.7 | 14.9 | 2.3 | 84.7 |
Amorphous Mo3VOx | 2.8 | 5.7 | 11.4 | 10.9 | 86.7 | 12.3 | 1.0 | 85.0 |
Tetragonal Mo3VOx | 0 | 2.7 | Tr | 0.3 | — | — | — | — |
The amorphous material had a similar micropore adsorption capacity to the trigonal material. The amount adsorbed is reasonable as the number of empty heptagonal channels in the amorphous sample should be statistically lower than that of the crystallized material. The tetragonal material, which is constructed with the pentagonal unit but without heptagonal channels, showed no micropore adsorption at all. This result supports the inference that the heptagonal channel is responsible for the microporosity.
Fig. 6 Conversion (A) and selectivity (B) changes as a function of reaction temperature in the oxidative dehydrogenation of ethane over four distinct Mo3VOx catalysts, orthorhombic (lozenges), trigonal (squares), amorphous (circles) and tetragonal (triangles). |
The clear effect of the structure can be summarised as follows: unexpectedly, it was found that the trigonal Mo3VOx catalyst showed much less activity than that of the orthorhombic Mo3VOx catalyst, in spite of their similar structures. The amorphous Mo3VOx catalyst also showed far less activity and the tetragonal Mo3VOx catalyst was found to be almost inactive. The catalytic activity difference depending on the catalysts cannot be explained either by the chemical composition (Table 1) or by the difference of the external surface area which is the sum of the minor surface of cross-section and the major surface of the rod wall (Table 2).
The structural character can be said to impart the greatest effect. Both highly active and less active catalysts have the same structural units and the difference is only the arrangement, such that it can be considered whether the materials possess the heptagonal channel or not is determinative for the ethane oxidation activity. Table 2 lists the values of the micropore volume of each catalyst. The value exhibits not only microporosity resulting from the empty heptagonal channels but can also be a rough measure of the amount of the empty heptagonal channel site on the surface of the cross-section of the rods. When this value is taken as the measure, a relationship between the micropore volume and the ethane conversion is clearly observable from the values in Table 2, suggesting that the heptagonal channel plays a crucial role in the course of ethane oxidation.
In terms of selectivity, only a slight difference among the catalysts can be observed in Fig. 6B. Nevertheless, the ethane oxidation was carried out over the orthorhombic Mo3VOx catalyst at a different space velocity. The result is listed in Table 2. The ethane conversion naturally decreased from 56% to 20% upon increasing the space velocity (by decreasing the catalyst amount from 0.5 g to 0.1 g), while the selectivity to ethene increased and the selectivities of COx and acetic acid decreased remarkably. This conversion is comparable to that obtained over the trigonal Mo3VOx catalyst with 0.5 g, while it was found that the ethene selectivity is higher over the orthorhombic catalyst than over the trigonal catalyst. The lower selectivity of the trigonal catalyst might be due to the unstable three-membered octahedra site around the heptagonal channel.
All the above results clearly demonstrate that high-dimensional arrangement of the catalytic components, Mo, V and O, supported by the bulk structures with high crystallinity is responsible for the observed remarkable catalytic activity of the crystalline orthorhombic Mo3VOx for the oxidative dehydrogenation of ethane to ethene. Furthermore, the microporous property brought about by the heptagonal channel seems to significantly contribute to the activation of ethane molecules and also in attaining high ethene selectivity, as ethane is small enough to be adsorbed in the mouth of the heptagonal channel under catalytic reaction conditions. Presumably, the empty heptagonal channel mouth and near distorted octahedra of V and Mo construct catalytic active sites. The former provides an ethane adsorption site to increase the probability of a reaction of ethane with active lattice oxygen in the latter. This situation can explain high activity at low reaction temperatures as categorized in the third group and also high selectivity to ethene due to an electron rich ethene which may not have access to the active site where ethane activation takes place.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c2cy20444d |
This journal is © The Royal Society of Chemistry 2013 |