Abstract
Alloying is well-known to improve the dehydrogenation selectivity of pure metals, but there remains considerable debate about the structural and electronic features of alloy surfaces that give rise to this behavior. To provide molecular-level insights into these effects, a series of Pd intermetallic alloy catalysts with Zn, Ga, In, Fe and Mn promoter elements was synthesized, and the structures were determined usingin situX-ray absorption spectroscopy (XAS) and synchrotron X-ray diffraction (XRD). The alloys all showed propane dehydrogenation turnover rates 5-8 times higher than monometallic Pd and selectivity to propylene of over 90%. Moreover, among the synthesized alloys, Pd3M alloy structures were less olefin selective than PdM alloys which were, in turn, almost 100% selective to propylene. This selectivity improvement was interpreted by changes in the DFT-calculated binding energies and activation energies for C-C and C-H bond activation, which are ultimately influenced by perturbation of the most stable adsorption site and changes to the d-band density of states. Furthermore, transition state analysis showed that the C-C bond breaking reactions require 4-fold ensemble sites, which are suggested to be required for non-selective, alkane hydrogenolysis reactions. These sites, which are not present on alloys with PdM structures, could be formed in the Pd3M alloy through substitution of one M atom with Pd, and this effect is suggested to be partially responsible for their slightly lower selectivity.
Original language | English |
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Pages (from-to) | 5066-5081 |
Number of pages | 16 |
Journal | Chemical Science |
Volume | 11 |
Issue number | 19 |
DOIs | |
State | Published - May 21 2020 |
Externally published | Yes |
Funding
This paper is based upon work supported in part by the National Science Foundation under Cooperative Agreement No. EEC-1647722. Use of the advanced photon source was supported by the U.S. Department of Energy, Office of Basic Energy Sciences, under contract no. DE-AC02-06CH11357. MRCAT operations, beamline 10-BM and 10-ID, are supported by the Department of Energy and the MRCAT member institutions. The authors also acknowledge the use of the 9-BM and 11-ID-C beamline at the advanced photon source. Use of the Center for Nanoscale Materials, an Office of Science user facility, was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357. Use of the National Energy Research Scientic Computing Center is also gratefully acknowledged. This paper is based upon work supported in part by the National Science Foundation under Cooperative Agreement No. EEC-1647722. Use of the advanced photon source was supported by the U.S. Department of Energy, Office of Basic Energy Sciences, under contract no. DE-AC02-06CH11357. MRCAT operations, beamline 10-BM and 10-ID, are supported by the Department of Energy and the MRCAT member institutions. The authors also acknowledge the use of the 9-BM and 11-ID-C beamline at the advanced photon source. Use of the Center for Nanoscale Materials, an Office of Science user facility, was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357. Use of the National Energy Research Scientific Computing Center is also gratefully acknowledged.
Funders | Funder number |
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National Energy Research Scientific Computing Center | |
Office of Basic Energy Sciences | DE-AC02-06CH11357 |
National Science Foundation | 1647722, EEC-1647722 |
U.S. Department of Energy | |
Office of Science |