ArticlePeerJ2016
Towards a barrier height benchmark set for biologically relevant systems.
Article in PeerJ, 2016. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 8 papers.
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Who cites it
8 citing papers in PubMed.
- The influence of model building schemes and molecular dynamics sampling on QM-cluster models: the chorismate mutase case study.Physical chemistry chemical physics : PCCP · 2024Article
- Benchmarking Density Functional Theory Methods for Metalloenzyme Reactions: The Introduction of the MME55 Set.Journal of chemical theory and computation · 2023Article
- How to Compute Atomistic Insight in DFT Clusters: The REG-IQA Approach.Journal of chemical information and modeling · 2023Article
- Barrier Height Prediction by Machine Learning Correction of Semiempirical Calculations.The journal of physical chemistry. A · 2023Article
- Mechanistic Modeling of Monoglyceride Lipase Covalent Modification Elucidates the Role of Leaving Group Expulsion and Discriminates Inhibitors with High and Low Potency.Journal of chemical information and modeling · 2022Article
- Intermolecular interactions in the condensed phase: Evaluation of semi-empirical quantum mechanical methods.The Journal of chemical physics · 2017Article
- Benchmarking density functional tight binding models for barrier heights and reaction energetics of organic molecules.Journal of computational chemistry · 2017Article
- An investigation into the applicability of the semiempirical method PM7 for modeling the catalytic mechanism in the enzyme chymotrypsin.Journal of molecular modeling · 2017Article
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Authors and funding
4 authors.
Funding
Abstract
We have collected computed barrier heights and reaction energies (and associated model structures) for five enzymes from studies published by Himo and co-workers. Using this data, obtained at the B3LYP/6- 311+G(2d,2p)[LANL2DZ]//B3LYP/6-31G(d,p) level of theory, we then benchmark PM6, PM7, PM7-TS, and DFTB3 and discuss the influence of system size, bulk solvation, and geometry re-optimization on the error. The mean absolute differences (MADs) observed for these five enzyme model systems are similar to those observed for PM6 and PM7 for smaller systems (10-15 kcal/mol), while DFTB results in a MAD that is significantly lower (6 kcal/mol). The MADs for PMx and DFTB3 are each dominated by large errors for a single system and if the system is disregarded the MADs fall to 4-5 kcal/mol. Overall, results for the condensed phase are neither more or less accurate relative to B3LYP than those in the gas phase. With the exception of PM7-TS, the MAD for small and large structural models are very similar, with a maximum deviation of 3 kcal/mol for PM6. Geometry optimization with PM6 shows that for one system this method predicts a different mechanism compared to B3LYP/6-31G(d,p). For the remaining systems, geometry optimization of the large structural model increases the MAD relative to single points, by 2.5 and 1.8 kcal/mol for barriers and reaction energies. For the small structural model, the corresponding MADs decrease by 0.4 and 1.2 kcal/mol, respectively. However, despite these small changes, significant changes in the structures are observed for some systems, such as proton transfer and hydrogen bonding rearrangements. The paper represents the first step in the process of creating a benchmark set of barriers computed for systems that are relatively large and representative of enzymatic reactions, a considerable challenge for any one research group but possible through a concerted effort by the community. We end by outlining steps needed to expand and improve the data set and how other researchers can contribute to the process.
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