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. 2024 Jan 12;128(3):1049-1057.
doi: 10.1021/acs.jpcc.3c06053. eCollection 2024 Jan 25.

Combined DFT and Kinetic Monte Carlo Study of UiO-66 Catalysts for γ-Valerolactone Production

Affiliations

Combined DFT and Kinetic Monte Carlo Study of UiO-66 Catalysts for γ-Valerolactone Production

Thanh-Hiep Thi Le et al. J Phys Chem C Nanomater Interfaces. .

Abstract

Zr-based metal-organic frameworks (MOFs) are excellent heterogeneous porous catalysts due to their thermal stability. Their tunability via node and linker modifications makes them amenable for theoretical studies on catalyst design. However, detailed benchmarks on MOF-based reaction mechanisms combined with kinetics analysis are still scarce. Thus, we here evaluate different computational models and density functional theory (DFT) methods followed by kinetic Monte Carlo studies for a case reaction relevant in biomass upgrading, i.e., the conversion of methyl levulinate to γ-valerolactone catalyzed by UiO-66. We show the impact of cluster versus periodic models, the importance of the DF of choice, and the direct comparison to experimental data via simulated kinetics data. Overall, we found that Perdew-Burke-Ernzerhof (PBE), a widely employed method in plane-wave periodic calculations, greatly overestimates reaction rates, while M06 with cluster models better fits the available experimental data and is recommended whenever possible.

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Conflict of interest statement

The authors declare no competing financial interest.

Figures

Figure 1
Figure 1
MOF-catalyzed conversion of methyl levulinate to γ-valerolactone via catalytic hydrogen transfer.
Figure 2
Figure 2
Structure of UiO-66: (a) periodic model, (b) pristine cluster model, and (c) defective iPrO-bound cluster model. Atom legend: Zr = green, O = red, C = gray, and H = white.
Figure 3
Figure 3
Electronic energy profiles (in kcal·mol–1) of defective UiO-66 using cluster models at PBE-D3 level and periodic models at PBE-D2 level. R = (CH2)2CO2Me.
Figure 4
Figure 4
Gibbs energy profile of the extended mechanism at 403.15 K (in kcal·mol–1) of defective UiO-66 using cluster models at the PBE-D3 level.
Figure 5
Figure 5
Gibbs energy profiles of the extended mechanism at 403.15 K (in kcal·mol–1) of defective UiO-66 using cluster models at the M06-L, PBE0-D3, and M06 levels.
Figure 6
Figure 6
Gibbs energy barriers (in kcal·mol–1) for the mechanistic steps at the PBE-D3, M06-L, PBE0-D3, and M06 levels. All barriers are computed using the TS and the prior most stable intermediate.

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