Can we ever develop an ideal RNA force field? Lessons learned from simulations of the UUCG RNA tetraloop and other systems

dc.contributor.authorMlýnský, Vojtěch
dc.contributor.authorKührová, Petra
dc.contributor.authorPykal, Martin
dc.contributor.authorKrepl, Miroslav
dc.contributor.authorStadlbauer, Petr
dc.contributor.authorOtyepka, Michal
dc.contributor.authorBanáš, Pavel
dc.contributor.authorŠponer, Jiří
dc.date.accessioned2026-04-28T08:24:08Z
dc.date.available2026-04-28T08:24:08Z
dc.date.issued2025
dc.description.abstractMolecular dynamics (MD) simulations are an important and well-established tool for investigating RNA structural dynamics, but their accuracy relies heavily on the quality of the employed force field (ff). In this work, we present a comprehensive evaluation of widely used pair-additive and polarizable RNA ffs using the challenging UUCG tetraloop (TL) benchmark system. Extensive standard MD simulations, initiated from the NMR structure of the 14-mer UUCG TL, revealed that most ffs did not maintain the native state, instead favoring alternative loop conformations. Notably, three very recent variants of pair-additive ffs, OL3CP–gHBfix21, DES-Amber, and OL3R2.7, successfully preserved the native structure over a 10 × 20 μs time scale. To further assess these ffs, we performed enhanced sampling folding simulations of the shorter 8-mer UUCG TL, starting from the single-stranded conformation. Estimated folding free energies (ΔG°fold) varied significantly among these three ffs, with values of 0.0 ± 0.6, 2.4 ± 0.8, and 7.4 ± 0.2 kcal/mol for OL3CP–gHBfix21, DES-Amber, and OL3R2.7, respectively. The ΔG°fold value predicted by the OL3CP–gHBfix21 ff was closest to experimental estimates, ranging from −1.6 to −0.7 kcal/mol. In contrast, the higher ΔG°fold values obtained using DES-Amber and OL3R2.7 were unexpected, suggesting that key interactions are inaccurately described in the folded, unfolded, or misfolded ensembles. These discrepancies led us to further test DES-Amber and OL3R2.7 ffs on additional RNA and DNA systems, where further performance issues were observed. Our results emphasize the complexity of accurately modeling RNA dynamics and suggest that creating an RNA ff capable of reliably performing across a wide range of RNA systems remains extremely challenging. In conclusion, our study provides valuable insights into the capabilities of current RNA ffs and highlights key areas for future ff development.
dc.description.firstpage4183
dc.description.issue8
dc.description.lastpage4202
dc.description.sourceWeb of Science
dc.description.volume21
dc.identifier.citationJournal of Chemical Theory and Computation. 2025, vol. 21, issue 8, p. 4183-4202.
dc.identifier.doi10.1021/acs.jctc.4c01357
dc.identifier.issn1549-9618
dc.identifier.issn1549-9626
dc.identifier.urihttp://hdl.handle.net/10084/158507
dc.identifier.wos001396622000001
dc.language.isoen
dc.publisherAmerican Chemical Society
dc.relation.ispartofseriesJournal of Chemical Theory and Computation
dc.relation.urihttps://pubs.acs.org/doi/10.1021/acs.jctc.4c01357?src=getftr&utm_source=clarivate&getft_integrator=clarivate
dc.rights© 2025 The Authors. Published by American Chemical Society
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/
dc.subjectmolecular dynamics simulations
dc.subjectparticle mesh ewald
dc.subjectprotein interactions
dc.subjectribosomal-subunit
dc.subjectcrystal-structure
dc.subjectreplica exchange
dc.subjectmonovalent ions
dc.subjectbase stacking
dc.subjectparameters
dc.subjectwater
dc.titleCan we ever develop an ideal RNA force field? Lessons learned from simulations of the UUCG RNA tetraloop and other systems
dc.type.statusPeer-reviewed
dc.type.versionpublishedVersion
local.files.count1
local.files.size14606053
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