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. 2022 Mar 21;10(11):3567-3573.
doi: 10.1021/acssuschemeng.1c08021. Epub 2022 Mar 4.

Computational Mechanism of Methyl Levulinate Conversion to γ-Valerolactone on UiO-66 Metal Organic Frameworks

Affiliations

Computational Mechanism of Methyl Levulinate Conversion to γ-Valerolactone on UiO-66 Metal Organic Frameworks

Manuel A Ortuño et al. ACS Sustain Chem Eng. .

Abstract

Metal-organic frameworks (MOFs) are gaining importance in the field of biomass conversion and valorization due to their porosity, well-defined active sites, and broad tunability. But for a proper catalyst design, we first need detailed insight of the system at the atomic level. Herein, we present the reaction mechanism of methyl levulinate to γ-valerolactone on Zr-based UiO-66 by means of periodic density functional theory (DFT). We demonstrate the role of Zr-based nodes in the catalytic transfer hydrogenation (CTH) and cyclization steps. From there, we perform a computational screening to reveal key catalyst modifications to improve the process, such as node doping and linker exchange.

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Conflict of interest statement

The authors declare no competing financial interest.

Figures

Scheme 1
Scheme 1. Conversion of Methyl Levulinate (ML) into γ-Valerolactone (GVL) via Catalytic Transfer Hydrogenation
Figure 1
Figure 1
Representation of Zr-based nodes. Zr = dark green, O = red, H = white.
Figure 2
Figure 2
Computed structure 1 at defective UiO-66 MOF. The periodic structure was cropped for better visualization. The black square indicates a Zr vacant site. Zr = dark green, O = red, H = white.
Figure 3
Figure 3
Reaction mechanism of ML to GVL at defective UiO-66 with relative Gibbs energies (in eV). R = (CH2)2CO2Me.
Figure 4
Figure 4
Gibbs energy reaction profile (in eV) at defective UiO-66 with relative barriers for each step.
Figure 5
Figure 5
DFT-optimized TS structures. Relevant atoms are display in ball-and-stick format, the rest of them in tube format. Selected distances are shown in Å.
Figure 6
Figure 6
(a) Hf-, Ti-, and Ce-doped nodes and (b) relative Gibbs energy barriers (in eV) for selected models. Barriers are computed from the transition state to the previous most stable intermediate.
Figure 7
Figure 7
(a) Linker-modified nodes and (b) relative Gibbs energy barriers (in eV) for selected models. Barriers are computed from the transition state to the previous most stable intermediate.

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