Targeting RNA with Small Molecules using State-of-the-Art Methods Provides Highly Predictive Affinities of Riboswitch Inhibitors

17 October 2024, Version 1
This content is a preprint and has not undergone peer review at the time of posting.

Abstract

Targeting RNA with small molecules represents a promising yet relatively unexplored avenue for the design of new drugs. Nevertheless, challenges arise from the lack of computational models and techniques able to accurately model RNA systems, and predict their binding affinities to small molecules. Here, we tackle these difficulties by developing a tailored state-of-the-art approach for absolute binding free energy calculations of RNA-binding small molecules. To do so, we combine the advanced AMOEBA polarizable force field, which accounts for both accurate multipolar electrostatics and many-body effects, to the newly developed Lambda-Adaptive Biasing Force (Lambda-ABF) scheme associated to refined restraints allowing for efficient sampling. Furthermore, to capture the free energy barrier associated to challenging RNA conformational changes, we apply machine learning to identify effective collective variables in order to use them into further enhanced sampling simulations based on an evolution of metadynamics. Applying this computational protocol to a complex Riboswitch-like RNA target, we demonstrate quantitative predictions. These results pave the way for the routine application of free-energy simulations in RNA-targeted drug discovery, thus providing a significant reduction in their failure rate.

Keywords

RNA
small molecules
Alchemical free energy simulations
Enhanced sampling
Drug Design
multipolar and polarizable force field
Riboswitch-like RNA
HCV-IRES

Supplementary materials

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Additional figures S1-S24 showing the convergence plots of all alchemical simulations; tables S1 and S2, show the electrostatic and van der Waals decomposition of the Potential of Mean Force (PMF). Illustration of the atoms involved in the definition of the DBC restraint (Figure S25) as well as the contribution of these restraints to the free energy reported in Table S3. Figures S26 and S27 report the RMSD of the biased trajectory corresponding to the Apo/Holo conformational change and the associated PMF.
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