2005
DOI: 10.12921/cmst.2005.11.01.49-55
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Parametrization of 2-thiouracil and 4-thiouracil in CHARMM all-atom empirical force field

Abstract: A new set of force field parameters complementing the CHARMM27 all atom empirical force field for nucleic acids was developed for 2-thiouracil and 4-thiouracil, two naturally modified RNA bases. The new parameters allow for molecular modeling and molecular dynamics simulations of RNA containing 2-thiouracil and 4-thiouracil.

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Cited by 7 publications
(4 citation statements)
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“…MD simulations were performed using the program NAMD 2.9 ( 32 ) with the CHARM27 parameter set modified to include parameters for s 2 U ( 33 ). All simulations used periodic boundary conditions with Langevin dynamics and a Langevin piston ( 34 ) to maintain the temperature at 298.15 K (with a damping constant of 5 ps −1 ) and the pressure at 1 atm.…”
Section: Methodsmentioning
confidence: 99%
“…MD simulations were performed using the program NAMD 2.9 ( 32 ) with the CHARM27 parameter set modified to include parameters for s 2 U ( 33 ). All simulations used periodic boundary conditions with Langevin dynamics and a Langevin piston ( 34 ) to maintain the temperature at 298.15 K (with a damping constant of 5 ps −1 ) and the pressure at 1 atm.…”
Section: Methodsmentioning
confidence: 99%
“…Until recently, the systematic development and validation of the force field parameters for modified RNAs were neglected [5,[46][47][48][49][50][51][52][53][54][55] (http://www.pharmacy.manchester.ac.uk/ bryce/amber). Aduri et al [56] first attempted the systematic development of AMBER force field parameter sets for 107 naturally occurring RNA modifications.…”
Section: Introductionmentioning
confidence: 99%
“…The poor performance of the MM FC model might not be caused by the FC approximation per se (which is adequate for the neutral G and A ) but rather by the insufficiency of the charge parametrization procedure (based on protocols of refs and ) in the case of the DC. For example, the largest difference in the atomic partial charges between the neutral G and G •+ in the MM simulations occurs for atoms N9 (−0.15), H8 (+0.16), N3 (+0.19), O6 (+0.21), and C8 (+0.33).…”
Section: Resultsmentioning
confidence: 99%
“…To the best of our knowledge, no MM simulations of G or A DCs were performed previously; therefore, no parameters existed for the DCs in CHARMM. We constructed the atomic partial charges for the DC following the standard CHARMM protocol of MacKerell et al , First, charge density differences between the neutral base and DC atoms were determined by QM (DFT/B3LYP/aug-cc-pVDZ level of theory in Gaussian03). The differences were added to the CHARMM atomic charges of the neutral base, resulting in the initial guess for the DC charges.…”
Section: Methodsmentioning
confidence: 99%