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Importance of the Inclusion of Dispersion in the Modeling of Asphaltene Dimers
Modeling of asphaltenes presents many challenges, not least of which is their large size and the lack of definitive experimental structure information. However, a further fundamental issue of importance is the ability of the modeling methodology to accurately predict noncovalent interactions, partic...
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Published in: | Energy & fuels 2010-12, Vol.24 (12), p.6468-6475 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that cite this one |
Online Access: | Get full text |
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Summary: | Modeling of asphaltenes presents many challenges, not least of which is their large size and the lack of definitive experimental structure information. However, a further fundamental issue of importance is the ability of the modeling methodology to accurately predict noncovalent interactions, particularly dispersion (London) forces. The self-aggregation properties of asphaltenes are primarily driven by such interactions. Therefore, for a modeling approach to be insightful, dispersion must be accounted for. This point is illustrated in this work by examining the effect of dispersion on the conformer distribution for a series of asphaltene model dimers, including perylene bisimide-type molecules and for a model of Maya asphaltene. Inclusion of dispersion using dispersion-correcting potentials on standard density-functionals is shown to be critical to both structure and conformer population for these noncovalently bound dimers. For the Maya asphaltene, a previously postulated “open” structure is shown to be ca. 9 kcal/mol less stable than a conformer that allows for greater π−π overlap within its central archipelago-type moiety. This finding is in line with recent NMR work, which indicates that “closed” structures dominate for asphaltenes. N,N′-dimethyl-perylene bisimide dimer has a binding energy (BE) of up to 29 kcal/mol, while the more complex N,N′-(1-hexylheptyl)-perylene bisimide model is slightly less strongly bound (BE = 25 kcal/mol) since the large alkyl substituents restrict the ability of the extensive π-regions to overlap. Such conclusions cannot be drawn when methods that do not incorporate dispersion, e.g., the B3LYP density-functional, are used. |
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ISSN: | 0887-0624 1520-5029 |
DOI: | 10.1021/ef100797h |