催化学报  2017, Vol. 38 Issue (1): 13-19   PDF    
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本文作者相关文章
Liu Jiaxu
Wang Jilei
Zhou Wei
Miao Cuilan
Xiong Guang
Xin Qin
Guo Hongchen
Construction of an operando dual-beam fourier transform infrared spectrometer and its application in the observation of isobutene reactions over nano-sized HZSM-5 zeolite
Liu Jiaxua, Wang Jileia, Zhou Weia, Miao Cuilana, Xiong Guanga, Xin Qinb, Guo Hongchena     
a. Department of Catalytic Chemistry and Engineering & State Key Laboratory of Fine Chemicals, Dalian University of Technology, Dalian 116012, Liaoning, China ;
b. State Key Laboratory for Catalysis, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian 116023, Liaoning, China
Foundation Item: This work was supported by the National Natural Science Foundation of China (21603023), and the PetroChina Innovation Foundation, China (2014D-5006-0501)
* Corresponding author. Tel/Fax: +86-411-84986120;E-mail:hongchenguo@163.com.
Abstract: An operando dual-beam Fourier transform infrared (DB-FTIR) spectrometer was successfully de-veloped using a facile method. The DB-FTIR spectrometer is suitable for the real-time study of the dynamic surface processes involved in gas/solid heterogeneous catalysis under real reaction condi-tions because it can simultaneously collect reference and sample spectra. The influence of gas-phase molecular vibration and heat irradiation at real reaction temperatures can therefore be eliminated. The DB-FTIR spectrometer was successfully used to follow the transformation of isobutene over nano-sized HZSM-5 zeolite under real reaction conditions.
© 2016, Dalian Institute of Chemical Physics, Chinese Academy of Sciences.
Published by Elsevier B.V. All rights reserved.
Key words: Operando DB-FTIR     Gas-phase molecular vibration spectroscopy     Heat irradiation influence     Real-time spectrum     Real reaction condition     Heterogeneous catalysis     Aromatization     Nano-sized HZSM-5 zeolite    
一种双光束红外光谱及其在气固相多相催化反应实时原位表征中的应用
刘家旭a, 王吉垒a, 周微a, 苗翠兰a, 熊光a, 辛勤b, 郭洪臣a     
a. 大连理工大学化工与环境生命学部精细化工国家重点实验室, 辽宁大连 116024 ;
b. 中国科学院大连化学物理研究所催化基础国家重点实验室, 辽宁大连 116023
摘要:单光束红外光谱技术(原位傅立叶透射变换红外、原位漫反射红外和衰减全反射红外光谱技术)虽然已经用于气固相多相催化反应的原位表征中,但这些光谱在真实反应条件下会受到气体分子振动光谱和加热条件下产生的发射光谱的严重影响,不能实时获得催化剂表面的真实信息.另外,由于在真实的气固相多相催化反应过程中,催化剂本底的信息会随着反应时间的延长而发生变化,因此单光束红外光谱技术在扣除本底信息方面存在误差. 为了实现在反应条件下,实时、原位表征催化剂表面的状态,我们报道了一种双光束红外光谱表征技术.该技术包括双光束红外光谱系统及双光束红外反应池.其特征在于:实时双光束原位红外光谱系统由两台完全相同的红外光谱仪和双光束红外反应池组成.双光束红外反应池由完全相同的样品池和参考池连接而成,样品池和参考池处于同一水平线上分别对应于样品光谱仪和参考光谱仪,由计算机同步控制两台红外光谱仪,排除实时状态下的气体分子振动光谱干扰和加热条件下产生的发射光谱干扰.该技术可以对真实反应条件下的气固相多相催化反应进行实时原位表征.通过应用程序的关联可以实时、同步采集样品光束和背景光束谱图来得到催化剂表面物种随反应时间变化的真实信息.该技术克服了单光束红外光谱在原位多相催化反应表征方面的缺陷,使表征结果变得更加精确可靠.该技术还可以在变化的气相组分条件下,获得不同温度下、实时的催化剂表面活性中心、活性相和中间物种的信息. 采用上述双光束红外光谱仪对丁烯在纳米HZSM-5催化剂上芳构化反应过程进行了实时、原位观测,首次在实际反应条件下,观察到了异丁烯在纳米HZSM-5沸石的表面Brönsted酸中心上经历吸附、活化、聚合、环化等反应步骤生成芳烃的过程.
关键词双光束原位红外光谱     气相分子振动光谱     热辐射     实时光谱     多相催化     真实反应条件     芳构化     纳米HZSM-5分子筛    

Currently, in situ transmission IR spectroscopy (TIRS), diffuse reflectance infrared Fourier transform (DRIFT) spectroscopy, and Fourier transform infrared attenuated total reflection (FTIR/ATR) spectroscopy are very popular tools in the study of heterogeneous catalysis. These techniques provide molecular- level information related to the surface active sites and the species adsorbed on heterogeneous catalysts [1-15]. However, all of these commercial FTIR spectrometers operate in the single- beam (SB-FTIR) mode, and require the measurement of reference (background) spectra to remove variations caused by changes in background absorption and instrument conditions [16]. They are not suitable for real-time study of the dynamic processes involved in gas/solid heterogeneous catalysis because they cannot collect the reference and sample spectra simultaneously. Another major problem with SB-FTIR spectrometers is that they are strongly influenced by gas-phase molecular vibration and heat irradiation at high temperatures. However, there is an urgent need for real-time surface characterization methods in the field of heterogeneous catalysis [17]. This is because the fundamental understanding of heterogene-ous catalytic processes, and thus the rational design of advanced catalysts, requires information related to the transient species involved in the reaction. These transient species can be captured only under real reaction conditions. In principle, a dual-beam Fourier transform infrared spectrometer (DB-FTIR) could simultaneously eliminate the influence of both gas-phase molecular vibration and heat irradiation at real reaction temperatures. This technique is therefore expected to be a useful operando characterization method for heterogeneous catalysis.

Kuehl, Dignam and Debreczeny et al [16, 18, 19] have tried to develop a DB-FTIR spectrometer by redesigning the optical layout of a commercial spectrometer to simulate dual-beam conditions. However, this is too difficult to be of practical use. To the best of our knowledge, the application of DB-FTIR in heterogeneous catalysis has not been reported until now.

Here, we report for the first time a facile method for the development of an operando DB-FTIR spectrometer. First, a special high-temperature IR reactor cell with two identical cells (for the reference and sample) was designed. This IR reactor cell enables the simultaneous collection of reference spectra, which result from gas-phase molecular vibration and heat irradiation, in the reference cell (without catalyst), and of sample spectra, which result from not only gas-phase molecular vibration and heat irradiation but also the catalyst surface species, in the sample cell (with catalyst). Then, two identical commercial infrared spectrometers were coupled together to construct a DB-FTIR spectrometer. The DB-FTIR spectrometer can perform time-resolved collection of both reference and sample spectra, and thus produce real-time spectra of the catalyst surface species under real heterogeneous reaction conditions (continuous gas flow and temperatures of up to 550 ℃) by simultaneous subtraction of the reference spectra from the sample spectra.

In this study, the IR reactor cell was developed to have identical CaF2 windows to ensure total elimination of the background interference (Fig. 1). Two Nicolet 10 s infrared spectrometers equipped with mercury cadmium telluride (MCT) detectors were used to construct the DB-FTIR spectrometer (Fig. 2). Special software was designed to ensure that the two spectrometers collected the spectra simultaneously. The catalysts were pressed into self-supporting thin wafers (1 cm2) that were placed in the sample beam, and the reference beam was vacant. The sample was activated in the IR reactor cell at 400 ℃ for 4 h under vacuum (10−3 Pa), and the spectra were recorded at a resolution of 4 cm−1 with 64 scans in the region of = 4000-1000 cm−1. The intensities of the reference and sample beams were adjusted to the same level.

Fig. 1. Photograph of the high-temperature quartz IR reactor cell.
Fig. 2. Photograph of the operando dual-beam FTIR spectrometer.

First, the equivalence of the reference and sample cells of the in-situ reactor, and the synchronism of the two spectrometers making up the DB-FTIR instrument were confirmed under working conditions by a blank test, as shown in Fig. 3. The spectra in Fig. 3 indicate that, in the absence of the catalyst, the differential spectra of the sample and reference cells were essentially straight lines, independent of the temperature of the cells (r.t. or 400 ℃) and the atmosphere (still air or a flowing mixture of isobutene and nitrogen gas) used.

Fig. 3. Differential spectra of the sample and reference cells of the DB-FTIR spectrometer in the absence of the catalyst under the following conditions: (1) r. t. and still air, (2) 400 ℃ and still air, (3) r.t. and a flowing mixture of isobutene and nitrogen gas, and (4) 400 ℃ and a flowing mixture of isobutene and nitrogen gas.

To demonstrate the advantages of the DB-FTIR instrument as an operando spectrometer, an ordinary SB-FTIR spectrometer was compared with the DB-FTIR spectrometer by studying isobutene and isobutane adsorptions on nano-sized HZSM-5 zeolite (SiO2/Al2O3 molar ratio = 26, crystal size = 20-50 nm), as shown in Figs. 4 and 5. Fig. 4 shows that during the adsorption of isobutene, the DB-FTIR spectrum contained only four obvious absorption bands, which could be attributed to the species adsorbed on the surface of the zeolite. According to literature [13], the bands at 2959 and 2873 cm−1 are attributed to the asymmetric and symmetric C-H stretching vibrations of the -CH3 group, respectively. The band at 2934 cm−1 is associated with the asymmetric C-H stretching vibration of the -(CH2)- group, and the band at 2860 cm−1 is attributed to the symmetric C-H stretching vibration of the -(CH2)- group. In contrast, when the ordinary SB-FTIR spectrometer was used, the obtained spectrum exhibited interference from gas-phase molecular vibration absorptions. This interference included not only weak absorptions in the region of 3072-3099 cm−1, but also very strong absorptions in the region of 2800-3000 cm−1; the latter strong absorptions were directly overlaid on the absorption bands of the surface species. Similar results were observed with the DB-FTIR and SB-FTIR spectrometers when isobutane was used as the adsorbate. However, adsorption of the less basic isobutane is more difficult than adsorption of isobutene on the protonic zeolite, so the surface-adsorbed isobutane afforded considerably weaker IR absorption bands at 2960, 2933, 2872, and 2860 cm−1, as shown in the DB-FTIR spectrum in Fig. 5. Consequently, when the ordinary SB-FTIR spectrometer was used, the weak absorptions of the surface species were completely overwhelmed by the absorptions from gas-phase molecular vibrations. These two examples thus indicate that, owing mainly to the influence of the gas-phase molecular spectrum, it is difficult to obtain the correct spectrum of the catalyst surface species under real reaction conditions using an ordinary SB-FTIR spectrometer. In contrast, the spectrum is easily obtained from the DB-FTIR spectrometer because the influence of the gas-phase molecular vibrations is completely eliminated by simultaneous subtraction of the reference spectrum.

Fig. 4. FTIR spectra of isobutene adsorption on nano-sized HZSM-5 zeolite using (1) the DB-FTIR spectrometer and (2) an ordinary SB-FTIR spectrometer at 150 ℃. (3) SB-FTIR spectrum without the catalyst, at 0.1 MPa and in a flowing mixture of isobutene and nitrogen gas (6% isobutene ‒94% nitrogen), GHSV = 1080 h−1.
Fig. 5. FTIR spectra of isobutane adsorption on nano-sized HZSM-5 zeolite using (1, 1′) the DB-FTIR spectrometer and (2) an ordinary SB-FTIR spectrometer at 150 ℃, 0.1 MPa, and in the flowing mixture of isobutane and nitrogen gas (6% isobutene ‒94% nitrogen), GHSV = 1080 h−1.

To examine the possibility of using the DB-FTIR spectrometer in a real-time operando study, it was used to follow the dynamic process of isobutene adsorption on nano-sized HZSM-5 at 150 ℃. Time-resolved spectra were collected at intervals of 1.27 min. Fig. 6 shows that at the beginning of the adsorption (first 4 min), three absorption bands were observed on the catalyst surface. The band at 3610 cm−1 is attributed to the bridging hydroxyl group (Si(OH)Al), that at 3726 cm−1 to free internal silanol (SiOH), and that at 3740 cm−1 to isolated external SiOH [20]. After 6.35 min, the band corresponding to the bridging hydroxyl group disappeared, and five new bands appeared. The new bands at 2956, 2933, 2872, and 2860 cm−1 are attributed to C-H stretching vibrations. As mentioned above, the bands at 2956 and 2872 cm−1 are respectively attributed to asymmetric and symmetric C-H stretching of the -CH3 group, whereas those at 2933 and 2860 cm−1 are assigned to the asymmetric and symmetric C-H stretching vibrations of the -(CH2)- group, respectively. The band at 1467 cm−1 is attributed to the C-H bending vibration of the -(CH2)- group, and that at 1458 cm−1 to the asymmetric C-H bending vibration of the -CH3 group. With an increase in the adsorption time from 6.35 to 8.89 min, the intensities of these six absorption bands increased slightly. However, increasing the adsorption time beyond 8.89 min did not lead to any further changes in the intensities of the bands, and the isobutene adsorption can be considered to have reached equilibrium. There is thus no doubt that the operando DB-FTIR spectrometer can be used to study dynamic surface processes in gas/solid heterogeneous catalysis under real conditions.

Fig. 6. Selected three-dimensional FTIR profiles of isobutene adsorption on nano-sized HZSM-5 zeolite at 150 ℃ and 0.1 MPa using a DB-FTIR spectrometer in a flowing mixture of isobutene and nitrogen gas (6% isobutene ‒94% nitrogen), GHSV = 1080 h−1.

Furthermore, the operando DB-FTIR spectrometer was used to study isobutene transformation over the nano-sized HZSM-5 zeolite at 300 ℃. Fig. 7 shows the spectra of the surface species on the catalyst in the first 15.24 min of the reaction (spectra collected at 1.27-min intervals). The bridging hydroxyl groups can be observed in the first 3.81 min, but their intensities clearly decrease with time. In the 3000-3100 cm−1 region, three bands were observed at 3080, 3085, and 3092 cm−1. These bands are ascribed to the =C-H stretching vibration of an aromatic ring [13]. In addition, an absorption band consisting of many overlapping signals, and thus caused by many different adsorbates, appears in the C-H stretching region (2800-3000 cm−1). This band is much stronger than the bands observed between 3000 and 3100 cm−1. There are three major absorption bands in the C-H bending region (1400-1600 cm−1). Among these, the band at 1505 cm−1 is related to the aromatic ring [13]. These spectra suggest that isobutene aromatization occurred very easily over the nano-sized HZSM-5 zeolite, even though the reaction temperature was as low as 300 ℃.

Fig. 7. Selected three-dimensional FTIR profiles of isobutene adsorption on nano-sized HZSM-5 zeolite at 300 ℃ and 0.1 MPa obtained using a DB-FTIR spectrometer in a flowing mixture of isobutene and nitrogen gas (6% isobutene ‒94% nitrogen), GHSV = 1080 h−1.

Fig. 8 shows the spectra of the surface species on the catalyst over a wide time span of 0-50 min. As the reaction time increases, the intensities of the absorption bands related to the aromatic ring, namely the C-H stretching vibrations at 3070, 3085, and 3091 cm−1, and the C-H bending vibration at 1505 cm−1, gradually increase. This means that isobutene aromatization over nano-sized HZSM-5 zeolite was enhanced at prolonged reaction time. Furthermore, the highly overlapped absorption band in the C-H stretching region at 2800-3000 cm−1 becomes stronger and wider as the reaction time increases. This band is most likely ascribed to various aromatic intermediates, which implies that multiple intermediates in the aromatization of isobutene were observed at the same time by the DB-FTIR spectrometer. These intermediates might help to establish a pool of precursors for the formation of aromatics. The observation of these intermediates agrees with the accepted viewpoint that the aromatization of olefins proceeds through a number of intermediates and carbenium ion transition states. This process involves the oligomerization-cracking of small olefins to give C4-C10 olefins, hydrogen transfer from the bigger olefins to the smaller olefins (mainly C2-C3) to give dienes, cyclization of the dienes to give cycloalkenes, and finally hydrogen transfer from the cycloalkenes to the small olefins to form the aromatic products [21-25]. Development of a precursor pool is likely to accelerate the formation of aromatics.

Fig. 8. Complete three-dimensional FTIR profiles of isobutene adsorption on nano-sized HZSM-5 zeolite at 300 ℃ and 0.1 MPa, obtained using a DB-FTIR spectrometer in a flowing mixture of isobutene and nitrogen gas (6% isobutene ‒94% nitrogen), GHSV = 1080 h−1.

As expected, when the DB-FTIR spectrometer was replaced with an ordinary SB-FTIR spectrometer to study the same isobutene transformation process, no valuable information was obtained concerning the surface changes (Fig. 9). In addition to the interference from the gas-phase molecular vibration absorptions, a strong effect of the heat irradiation on the bending vibrations of the C-H bonds (1400-1600 cm−1) was also observed at the high reaction temperature (300 ℃).

Fig. 9. Selected three-dimensional FTIR profiles of isobutene desorption at 300 ℃ from nano-sized HZSM-5 zeolite, obtained using a SB-FTIR spectrometer. Isobutene (6%, nitrogen balanced) adsorption at a flow rate of 3 mL/min for 0.5 h at 150 ℃ ensured saturated adsorption. The sample was then purged with N2 at a flow rate of 10 mL/min at 300 ℃, 0.1 MPa.

In summary, an operando DB-FTIR spectrometer has been developed for the first time using a facile method. This spectrometer is expected to be a powerful tool for the in-situ study of heterogeneous catalysis. It is very convenient for eliminating the effects of gas-phase molecular vibration and heat irradiation, and can provide important information on surface active sites, intermediate or spectator species and the reaction mechanism under real reaction conditions. Further work on the dynamic processes of several important reactions involving heterogeneous catalysis, including the aromatization of short-chain alkanes over HZSM-5 and Zn/HZSM-5 zeolite, is currently underway in our group.

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