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Volumn 16, Issue 1, 1998, Pages 139-143

Stabilization of the purine•purine•pyrimidine dna base triplets by divalent metal cations

Author keywords

[No Author keywords available]

Indexed keywords

DIVALENT CATION; DNA; MAGNESIUM; PURINE; PURINE DERIVATIVE; PYRIMIDINE; PYRIMIDINE DERIVATIVE; ZINC; ADENINE; CYTOSINE; GUANINE; HYDROGEN; METAL ION; THYMINE;

EID: 0031593720     PISSN: 07391102     EISSN: 15380254     Source Type: Journal    
DOI: 10.1080/07391102.1998.10508235     Document Type: Article
Times cited : (45)

References (18)
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    • Basch, H., Krauss, M., and Stevens, W. J., 1985. J. Am.Chem.Soc., 107:7267–7271. (a) (b). E.H.S. Anwander, M.M. Probstand B.M. Rode,. Biopolymers 29, 757–769 (1990);(c). J. Šponer, J.V. Burda, P. Mejzlik, J. Leszczynski and P. Hobza, J. Biomol. Struct. Dynamics 14, 613–628 (1997)
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    • 11 as in our previous studies (12). The interaction energies were evaluated for the HF-optimized geometries by using the full second-order Moeller-Plesset perturbational method (MP2). The main task of the present study was to estimate the influence of the solvated metal cation on the stability of the purine-purine base pairs. Therefore, the remote pyrimidine base was neglected in the calculation of interaction energies, as this base does not have any significant effect on the purine-purine interaction. The cation with its hydration sphere was considered as one subsystem. Thus, the energy calculations were performed for the purine-purine-hydrated cation “trimer”. The energy of interactions within the trimer was decomposed into the individual pair wise contributions and a three-body term. (9c, 12b, c). The interaction energies were corrected for the basis set superposition error (13) in the trimer-centered basis set. All of the calculations were done by using the Gaussian 94 suite of programs (14)
    • 11 as in our previous studies (12). The interaction energies were evaluated for the HF-optimized geometries by using the full second-order Moeller-Plesset perturbational method (MP2). The main task of the present study was to estimate the influence of the solvated metal cation on the stability of the purine-purine base pairs. Therefore, the remote pyrimidine base was neglected in the calculation of interaction energies, as this base does not have any significant effect on the purine-purine interaction. The cation with its hydration sphere was considered as one subsystem. Thus, the energy calculations were performed for the purine-purine-hydrated cation “trimer”. The energy of interactions within the trimer was decomposed into the individual pair wise contributions and a three-body term. (9c, 12b, c). The interaction energies were corrected for the basis set superposition error (13) in the trimer-centered basis set. All of the calculations were done by using the Gaussian 94 suite of programs (14)
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    • 2+ system without inclusion of the BSSE corrections. The uncorrected value of the interaction energy is −147.4 kcal/mol, ca.18 kcal/mol lower than the BSSE-corrected value in Table I. Thus, in contrast to the popular belief that BSSE is quite negligible for ionic systems, the correction is quite significant and we recommend correcting all data for larger systems by applying the countepoise procedure
    • 2+ system without inclusion of the BSSE corrections. The uncorrected value of the interaction energy is −147.4 kcal/mol, ca.18 kcal/mol lower than the BSSE-corrected value in Table I. Thus, in contrast to the popular belief that BSSE is quite negligible for ionic systems, the correction is quite significant and we recommend correcting all data for larger systems by applying the countepoise procedure
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    • The constraint has been applied for the following reason: during the optimization the structure was essentially planar for approximately 20 cycles, followed by a rotation and pyramidalization of the proximal amino group with a subsequent very fast disruption of the AA base pairving in the A.AT triplet. The unconstrained optimization was then terminated because the resulting structure was not compatible with the H-bonded arrangement of bases in the triplet. (Similar behavior was observed for unconstrained optimizations of the bare metal ion—;AA rH systems).9c
    • The constraint has been applied for the following reason:during the optimization the structure was essentially planar for approximately 20 cycles, followed by a rotation and pyramidalization of the proximal amino group with a subsequent very fast disruption of the AA base pairving in the A.AT triplet. The unconstrained optimization was then terminated because the resulting structure was not compatible with the H-bonded arrangement of bases in the triplet. (Similar behavior was observed for unconstrained optimizations of the bare metal ion—;AA rH systems).9c
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    • hydr contributions. For more details see ref. 12c
    • hydr contributions. For more details see ref. 12c
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