Xiaoming Hua,
Mengwen Huanga,
Tetsuya Kinjyob,
Shinya Minec,
Takashi Toyaoa,
Yoyo Hinumad,
Masaaki Kitanoef,
Toyoto Satog,
Norikazu Namikib,
Ken-ichi Shimizua and
Zen Maeno*b
aInstitute for Catalysis, Hokkaido University, N-21, W-10, Sapporo 001-0021, Japan
bSchool of Advanced Engineering, Kogakuin University, 2665-1, Nakano-cho, Hachioji, 192-0015, Japan. E-mail: zmaeno@cc.kogakuin.ac.jp
cNational Institute of Advanced Industrial Science and Technology (AIST), Research Institute for Chemical Process Technology, 4-2-1 Nigatake, Miyagino, Sendai 983-8551, Japan
dDepartment of Energy and Environment, National Institute of Advanced Industrial Science and Technology, 1-8-31, Midorigaoka, Ikeda 563-8577, Japan
eMDX Research Center for Element Strategy, International Research Frontiers Initiative, Tokyo Institute of Technology, Midori, Yokohama 226-8503, Japan
fAdvanced Institute for Materials Research (WPI-AIMR), Tohoku University, Sendai 980-8577, Japan
gDepartment of Engineering Science and Mechanics, College of Engineering, Shibaura Institute of Technology, Tokyo 135-8548, Japan
First published on 25th July 2024
Catalytic propane dehydrogenation (PDH) has mainly been studied using metal- and metal oxide-based catalysts. Studies on dehydrogenation catalysis by metal hydrides, however, have rarely been reported. In this study, PDH reactions using group IIIB and IVB metal hydride catalysts were investigated under relatively low-temperature conditions of 450 °C. Lanthanum hydride exhibited the lowest activation energy for dehydrogenation and the highest propylene yield. Based on kinetics studies, a comparison between the reported calculation results and isotope experiments, the hydrogen vacancies of metal hydrides were involved in low-temperature PDH reactions.
Catalytic applications of hydrogen-containing compounds have been a topic of interest in catalysis research.21–25 Several metal hydrides and hydrogen-containing mixed-anion compounds are effective catalysts and/or supports for the hydrogenation of CO2 and N2, with lattice hydrogen atoms and/or hydrogen vacancies playing an important role.26–34 However, their effectiveness in dehydrogenation has not been reported since early studies were conducted in the 1920s–1950s.35,36 Recently, our group reported that titanium hydrides exhibit a superior propylene formation rate compared to that achieved using titanium oxides at 450 °C.37 As a continuation of that study, we investigated the PDH reaction over group IIIB (Sc, Y, and La) and IVB (Ti, Zr, and Hf) metal hydrides, all of which showed higher activity compared to that exhibited by the corresponding metal oxides at 450 °C. Among the tested metal hydrides, lanthanum hydride afforded the highest propylene yield. Notably, the activation barrier for PDH using lanthanum hydride was 34.6 kJ mol−1, which is much lower than those using PtSn and CrOX catalysts. The involvement of hydrogen vacancies in metal hydrides in low-temperature PDH reactions is also discussed.
To investigate the temperature-dependency of formation rate, the PDH reaction was carried out under the following conditions: 100 mg of catalysts, 10 mL min−1 of 10% C3H8/He, 430–460 °C for metal hydrides, 410–440 °C for PtSn/SiO2 and CrOX–Al2O3. The average propylene formation rate at each temperature was used for data analysis. For the comparison among a series of metal hydrides, the propylene formation rate is calculated based on each mole of catalyst, while for the comparison of LaH3 with PtSn and CrOX catalysts, the propylene formation rate is calculated based on each gram of catalyst. For the effect of partial propane pressure, the reaction was performed under the following conditions: 100 mg of metal hydrides, 50 mL min−1 of 2–8% C3H8/He, 450 °C. For the effect of partial H2 pressure, the reaction was performed under the following conditions: 100 mg of metal hydrides, 50 mL min−1 of 2–8% H2 + 10% C3H8/He, 450 °C.
Catalyst | Conv.a (%) | SC3H6a (%) | YC3H6a (%) |
---|---|---|---|
a Reaction conditions: 100 mg of catalyst, 10 mL min−1 of 10% C3H8/He, and 450 °C. Details of determination are described in Experimental section. | |||
ScH2 | 0.5 | >99.9 | 0.5 |
ScH2_BM | 8.3 | 36.6 | 3.1 |
Sc2O3 | 0.1 | 17.6 | <0.1 |
YH3 | 0.5 | 60.4 | 0.3 |
YH3_BM | 4.5 | 53.2 | 2.4 |
Y2O3 | <0.1 | 58.7 | <0.1 |
LaH3 | 0.6 | 88.8 | 0.5 |
LaH3_BM | 11.8 | 92.7 | 11.0 |
La2O3 | 0.4 | 34.8 | 0.1 |
TiH2 | 0.4 | 52.6 | 0.2 |
TiH2_BM | 1.5 | 82.6 | 1.2 |
TiO2_Anatase | 0.5 | 73.0 | 0.4 |
TiO2_Rutile | 0.7 | 96.1 | 0.7 |
ZrH2 | 0.2 | 90.5 | 0.2 |
ZrH2_BM | 1.9 | 86.6 | 1.7 |
ZrO2 | 0.4 | 47.7 | 0.2 |
HfH2 | 0.2 | 82.9 | 0.2 |
HfH2_BM | 2.5 | 81.8 | 2.0 |
HfO2 | 0.0 | 56.2 | 0.0 |
Fig. 1 YC3H6 and normalized formation rate based on surface area in PDH using group IIIB and IVB metal hydrides (ball-milled for 1 h) at 450 °C. |
Our previous study on PDH over TiH2 revealed that partially dehydrogenated titanium hydrides are more active than Ti metal.37 In this study, LaH3 was pre-treated under He flow at different temperatures to promote the desorption of lattice hydrogen and was then applied to the PDH reaction at 450 °C. The He treatments at 450 and 600 °C did not significantly affect the reaction, and thus similar YC3H6 values were obtained (0.5%, Fig. 2a). When the pre-treatment temperature was increased to 700 and 800 °C, YC3H6 decreased to 0.3% and <0.1%, respectively. In the TPD of LaH3, a small desorption peak at 300–500 °C and a larger peak at 700–800 °C were observed (Fig. 2b). The loss of activity by high temperature pretreatment is possibly deep dehydrogenation of LaH3 to La metal. To discuss this consideration, we conducted H2 TPD of LaH3 up to 800 °C to completely release hydrides and then successively investigated H2 temperature programmed reduction (TPR) to study the H2 absorption property. The main H2 absorption peak was observed from 300–400 °C (Fig. S5†). The H2-treated sample showed the intermediate YC3H6 value (0.3%), which was lower than that of fresh LaH3 (0.5%) and higher than Ar-treated one (<0.1%), supporting the above consideration.
The XRD measurements of LaH3 before and after PDH at 450 °C showed that the diffraction peaks shifted toward lower angles after the reaction (Fig. S6†). A decrease in hydrogen content induces lattice expansion in the lanthanum hydride system.38 To study the change of lattice constant in detail, the synthesized LaH3 was treated under argon or propane (1 atm) atmosphere at 450 °C in a batch reactor, and then the treated samples were characterized by XRD with using Si powder as an internal standard (Fig. 3a and b). Using indexing program TREOR97 and least-squares refinement of lattice constant program PIRUM (see ESI†), observed Bragg peaks of as-prepared sample were indexed by a pseudo-cubic unit cell with a = 5.6119(11) Å, which corresponds to H/La = 2.77 as estimated by comparison with calculated lattice constant of LaH3 and LaH2 (Fig. 3c), showing the formation of relatively highly-hydrogenated lanthanum hydrides. The treatment under argon (as an inert gas) induced the increase of lattice constant to 5.6188(8) Å (the pseudo-cubic unit cell), and the propane treatment resulted in the further slightly increase to 5.6246(4) Å (the pseudo-cubic unit cell). The estimated H/La values were 2.61 and 2.49, respectively. These results show that the formation of hydrogen vacancy mainly occurred by thermal treatment and indicate that the incorporation of hydrogen derived from propane into the generated vacancy is unlikely to occur during PDH.
We also investigated the PDH using LaH3 under higher space velocity conditions (100 mL min−1 of 10% C3H8/Ar). The detailed results including the carbon balance value were shown in Table S1.† Although the initial conversion was relatively high (15.4%), the SC3H6 value was quite low owing to cracking reaction and the carbon balance was moderate (60%), resulting in a low YC3H6. The conversion decreased to 2–3% whereas was good SC3H6 and carbon balance values was maintained. The used catalyst was treated with H2 at 300 °C to try to regenerate the initial activity. Unfortunately, the initial activity was not recovered (Table S2†), indicating that deep dehydrogenation is unlikely to cause the deactivation. The specific surface area of the used ball-milled LaH3 was 6.5 m2 g−1, which was similar to the original one (7.5 m2 g−1), indicating that the sintering was unlikely to occur. Because the carbon balance value at initial stage was relatively low in PDH using fresh LaH3, the coke formation is more plausible reason for deactivation.
The temperature dependence of the propylene formation rate using different metal hydrides was plotted, and the apparent activation energies (Ea) were compared. TiH2 was excluded because the Ea value is too dependent on H2 co-feeding due to the interconversion between titanium hydride and Ti metal.37 The Ea values for the group IIB metal hydrides were lower than those for the group IVB metal hydrides (Fig. 4a). LaH3 exhibited the lowest Ea (34.6 kJ mol−1), whereas the highest Ea (147.5 kJ mol−1) was observed for HfH2. Notably, under low-temperature conditions, the Ea for LaH3 is lower than those for PtSn- and CrOX-based catalysts (74.0 and 94.0 kJ mol−1, respectively), as shown in Fig. 4b. In addition, industrially used K–PtSn/Al2O3 was prepared according to the previous report and investigated kinetic study. The Ea value (117 kJ mol−1) was higher than that for LaH3 (Fig. S7†), indicating the high catalytic potential of LaH3.
Fig. 4 Temperature dependence of propylene formation rate in PDH using (a) a series of metal hydrides and (b) PtSn- and CrOX-based catalysts. |
In previous studies on PDH over group IVB metal oxides, such as TiO2 and ZrO2, oxygen vacancies generated by H2 or CO pre-treatment were involved in C–H bond cleavage, promoting PDH.15,16 In this study, we discuss the possible involvement of hydrogen vacancies during PDH based on partial pressure changes and the relationship between activity and the formation energy of surface hydrogen vacancies. The effects of the partial pressures of propane and H2 (p(C3H8) and p(H2)) on PDH using LaH3 were investigated. The reaction order of p(H2) was determined to be approximately −0.5, whereas the reaction order of p(C3H8) was relatively low and positive (approx. 0.2) (Fig. 5). Similar partial pressure effects were observed in the PDH using another metal hydride (Fig. S8†). Interestingly, the PtSn-based catalyst system exhibited a zero-order dependency on p(H2).39,40 It can be considered that an increase in p(H2) suppresses the formation of hydrogen vacancies, resulting in a decreased propylene formation rate. The initial YC3H6 values are plotted as a function of theoretical formation energies of the surface hydrogen vacancies (EHvac).41 As EHvac decreased, the initial YC3H6 increased, and the lanthanum hydrides possessing the lowest EHvac exhibited the highest YC3H6 (Fig. 6). These results imply that hydrogen vacancies in metal hydrides are involved in the PDH reaction.
Fig. 6 Correlation of initial YC3H6 with theoretical formation energy of surface hydrogen vacancies (E_Hvac) for group IIIB and IVB metal hydrides.41 |
To further investigate the involvement of hydrogen vacancies, LaD3 was prepared from a lanthanum chip and D2 gas for testing in the PDH reaction. The generated gas products, including H2, HD, and D2, were monitored using mass spectrometry (m/z = 2, 3, and 4, respectively) and then compared with the PDH reactions using LaH3. During the pre-treatment of LaH3 under Ar flow, H2 desorption occurred as the temperature was increased from room temperature to 450 °C (Fig. S9†), indicating the generation of hydrogen vacancies under PDH reaction conditions. After the introduction of propane at 450 °C, H2 was formed, and D2 and HD were barely detected (Fig. 7a). When LaD3 was used instead of LaH3, D2 desorption was observed during a similar pre-treatment under Ar flow (Fig. S9†). In the PDH reaction, D2 and HD were simultaneously formed, and the signal intensity for H2 was much lower than that observed when using LaH3 (Fig. 7b). In a separate experiment, LaD3 exhibited PDH activity, in which the time course of YC3H6 was similar to that obtained when using LaH3 (Fig. S10†). These results indicate that the H atoms of C3H8 are incorporated into the hydrogen vacancies of LaD3 and then exchanged/combined with lattice D atoms, resulting in the formation of D2/HD as co-products. To determine whether an exchange reaction occurred between LaD3 and the gas-phase H2, the H–D exchange reaction of LaD3 with H2 was also conducted at 450 °C. The peak for D2 immediately appeared after Ar pre-treatment and the introduction of H2, while the signals for HD and H2 were hardly detected directly after the introduction of H2. With a decreasing signal for D2, a peak for HD formation was observed, and the signal intensity for H2 increased (Fig. S11†). This observation was different from that of the PDH reaction, suggesting that the exchange reaction of LaD3 with H2 was not a plausible formation pathway for D2 or HD. These isotope experiments provide further indicate for the involvement of the hydrogen vacancies in LaH3 in PDH reactions.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ra02473g |
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