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Microhydration of guanine...cytosine base pairs, a theoretical study on the role of water in stability, structure and tautomeric equilibrium
T. Zelený, P. Hobza, M. Kabeláč
Language English Country Great Britain
- MeSH
- Cytosine chemistry MeSH
- DNA chemistry MeSH
- Financing, Organized MeSH
- Guanine chemistry MeSH
- Isomerism MeSH
- Nucleic Acid Conformation MeSH
- Quantum Theory MeSH
- Models, Molecular MeSH
- Base Pairing MeSH
- Computer Simulation MeSH
- Thermodynamics MeSH
- Water chemistry MeSH
The potential energy surfaces of guanine...cytosine complexes and microhydrated guanine...cytosine (one and two water molecules) were investigated by the molecular dynamics/quenching method (MD/Q), using the empirical potential Parm94 force field, implemented in the Amber program package. The calculations were conducted for all the possible combinations of the four most stable tautomers of guanine and three of cytosine (covering the canonical forms in both cases). The obtained structures were sorted by their structural motifs into three main groups: planar hydrogen-bonded; stacked; and T-shaped structures. The most stable structures found at the empirical potential energy surfaces were fully reoptimised at the second-order Moller-Plesset perturbation theory as well as using the density functional method with an empirical dispersion term (DFT-D). A combination of the canonical form of guanine and cytosine and canonical cytosine with a guanine tautomer where the hydrogen is switched from position N9 to N7 are energetically preferred in microsolvated systems as well as those without the presence of a solvent. The rising number of water molecules leads to smaller differences between the stability of the various combinations of the tautomers of bases in the base pairs. For some of the tautomer combinations (mainly the enol-enol combination), two water molecules are sufficient for the preference of stacked structures over the H-bonded ones. The interaction energies and geometries obtained by the second-order Moller-Plesset perturbation theory method and the much less computationally demanding DFT-D method are comparable, except for stacked complexes, where the interaction energies are overestimated on average by 3 kcal mol(-1) at the MP2 level.
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- $a Department of Physical Chemistry, Faculty of Sciences, Palacky University, tr. Svobody 26, 771 46, Olomouc, Czech Republic. tomas.zeleny@upol.cz
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- $a The potential energy surfaces of guanine...cytosine complexes and microhydrated guanine...cytosine (one and two water molecules) were investigated by the molecular dynamics/quenching method (MD/Q), using the empirical potential Parm94 force field, implemented in the Amber program package. The calculations were conducted for all the possible combinations of the four most stable tautomers of guanine and three of cytosine (covering the canonical forms in both cases). The obtained structures were sorted by their structural motifs into three main groups: planar hydrogen-bonded; stacked; and T-shaped structures. The most stable structures found at the empirical potential energy surfaces were fully reoptimised at the second-order Moller-Plesset perturbation theory as well as using the density functional method with an empirical dispersion term (DFT-D). A combination of the canonical form of guanine and cytosine and canonical cytosine with a guanine tautomer where the hydrogen is switched from position N9 to N7 are energetically preferred in microsolvated systems as well as those without the presence of a solvent. The rising number of water molecules leads to smaller differences between the stability of the various combinations of the tautomers of bases in the base pairs. For some of the tautomer combinations (mainly the enol-enol combination), two water molecules are sufficient for the preference of stacked structures over the H-bonded ones. The interaction energies and geometries obtained by the second-order Moller-Plesset perturbation theory method and the much less computationally demanding DFT-D method are comparable, except for stacked complexes, where the interaction energies are overestimated on average by 3 kcal mol(-1) at the MP2 level.
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