MOFs & Structures: How does Changing the Metal Affect CO2 Uptakes

MOFs are tunable materials with potential for CO2 capture. Interestingly, MOFs with the same metal and ligand can form different structures due to experimental conditions, while distinct components may yield identical structures. How do these features impact their performance for CO2 capture?
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Designing materials for efficient carbon capture requires careful design and expertise. Due to their high tunability, selectivity, and porosity, metal-organic frameworks (MOFs) are promising candidates for CO2 capture. However, challenges still lie in predicting which MOF will perform reliably, especially when moving from computer simulations to real-world synthesis and testing. Screenings on large datasets are a promising avenue as they are generally much faster and more efficient than any group of scientists in a wet lab. However, experimentally verifying computational results is often the pitfall of such projects.

In our recent study, we systematically investigated a family of pyrene-based MOFs for carbon capture, each incorporating a different metal: aluminum (Al), gallium (Ga), indium (In), and scandium (Sc). These materials are expected to crystallize in an orthorhombic space group, where infinite metal rods hold the pyrene ligand in a stacking fashion, creating a very promising active site for CO2 uptake from wet flue gas1. While the ligand remains unchanged (i.e., 1,3,6,8-tetrakis(p-benzoic acid)pyrene (TBAPy)), computational predictions suggested that the choice of metal incorporated would significantly influence the stacking distance between pyrene layers1. Such structural variations would directly impact the CO2 uptake of the material, highlighting its critical role in tuning adsorption properties. This was the case for Al-TBAPy1 and Sc-TBAPy2, which maintain the orthorhombic crystal structure. However, In-TBAPy3 and Ga-TBAPy4,5 reveal the presence of additional phases. As reported in its original publication, although In-TBAPy crystallizes in an orthorhombic structure, upon activation and solvent removal from the pores, it transitions to a monoclinic phase3. On the other hand, Ga-TBAPy crystallizes in a monoclinic space group and maintains this structure throughout activation (although a secondary orthorhombic phase also seems to coexist). The Ga-TBAPy structure was solved via micro-electron diffraction (microED/3D-ED), as single crystals were not obtained. The monoclinic structure no longer shows the perfect stacking of the TBAPy ligand as observed in their orthorhombic counterpart (Figure 1).  A rotation of the benzoate groups of the ligand results in a break-up of the linear arrangement of the metal ions, which subsequently leads to a shift of the ligand in the structure. This phenomenon leads to a clear change of the CO2 binding site, as the pyrene stacks are no longer parallel and much shorter, making it impossible for CO2 to be adsorbed there.

Orthorhombic and monoclinic structures investigated in this study, highlighting the pyrene stacks for preferential CO2 binding (i.e., site A), as well as pores B and C.

Integrated lab and computer experiments were also performed. In that regard, we developed four computational models for the orthorhombic structures and two monoclinic models for the In- and Ga-TBAPy structures. Computational CO2 adsorption isotherms show that the monoclinic structures saturate at much lower pressures than the orthorhombic structures, possibly due to their much lower pore volume. Experimentally, in the low-pressure regime, the uptakes match more closely to the uptakes of the simulated monoclinic structures. At the same time, at higher pressure, they follow more closely the orthorhombic ones, which may suggest structural rearrangements upon CO2 loading (Figure 2).

Experimental and computational CO2 isotherms of the M-TBAPy MOFs discussed in this study.

A mixed-metal Al0.50Sc0.50-TBAPy MOF is also synthesized, as these are the only precursors maintaining the orthorhombic phase before and after activation at the reported conditions. In silico structures with different Al vs Sc arrangements are developed, showing that different metal configurations do not significantly affect this structure's uptake.

Further analysis may be needed to uncover the underlying details fully, but we believe these structural variations affect the MOFs' gas adsorption properties. Accounting for these phases may improve the accuracy of predicted adsorption isotherms, more easily bridging the gap between simulations and experiments.

Feel free to explore the complete study on evaluating and fine-tuning MOF structures for CO2 adsorption at: https://www.nature.com/articles/s41467-025-56296-w.

References:

1. Boyd, P. G.; Chidambaram, A.; García-Díez, E.; Ireland, C. P.; Daff, T. D.; Bounds, R.; G ladysiak, A.; Schouwink, P.; Moosavi, S. M.; Maroto-Valer, M. M.; others Data-driven design of metal–organic frameworks for wet flue gas CO2 capture. Nature 2019, 576, 253–256.

2. Kinik, F. P.; Ortega-Guerrero, A.; Ebrahim, F. M.; Ireland, C. P.; Kadioglu, O.; Mace, A.; Asgari, M.; Smit, B. Toward Optimal Photocatalytic Hydrogen Generation from Water Using Pyrene-Based Metal-Organic Frameworks. ACS applied materials & interfaces 2021, 13, 57118–57131.

3. Stylianou, K. C.; Heck, R.; Chong, S. Y.; Bacsa, J.; Jones, J. T.; Khimyak, Y. Z.; Bradshaw, D.; Rosseinsky, M. J. A guest-responsive fluorescent 3D microporous metal-organic framework derived from a long-lifetime pyrene core. Journal of the American Chemical Society 2010, 132, 4119–4130.

4. Patricio Domingues, N. Understanding & Application Driven Design of Metal-Organic Frameworks for Carbon Capture. Infoscience EPFL Scientific Publications 2021.

5. Ahlén, M.; Zhou, Y.; Hedbom, D.; Cho, H. S.; Strømme, M.; Terasaki, O.; Cheung, O. Efficient SF6 capture and separation in robust gallium-and vanadium-based metal–organic frameworks. Journal of Materials Chemistry A 2023, 11, 26435–26441.

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