Structural equilibrium of DNA represented with different force fields

Change in conformation by DNA-peptide association: molecular dynamics of the Hin-recombinase-hixL complex

The Hin-DNA complex is a molecular complex formed by the C-terminal 52mer peptide of the Hin-recombinase and a synthetic 13-bp hixL DNA. The peptide has three alpha-helices, the second and third of which form the helix-turn-helix motif to bind to the major groove. Both termini of the peptide reside within the minor groove. Three molecular dynamics simulations were performed based on the crystal structure of the Hin-DNA complex: one for the free Hin peptide, one for the free hixL DNA, and one for the complex. Analyses of the trajectories revealed that the dynamic fluctuations of both the Hin peptide and the hixL DNA were lowered by the complex formation. The simulation supported the experimental observation that the N-terminus and the helix-turn-helix motif were critical for formation of the complex, but the C-terminus played only a supportive role in DNA recognition. The simulations strongly suggested that the binding reaction should proceed by the induced fit mechanism. The ion and solvent distributions around the molecules were also examined.

DNA structure: cations in charge?

Recent X-ray diffraction, NMR spectroscopy and molecular mechanics results suggest that monovalent cations selectively partition into the minor groove of AT-tracts in DNA. These observations are consistent with DNA deformation by electrostatic collapse around areas of uneven cation density. This model predicts the occurrence of known DNA deformations, such as AT-tract bending and changes in the minor-groove width.

Intrinsic conformational properties of deoxyribonucleosides: implicated role for cytosine in the equilibrium among the A, B, and Z forms of DNA

Structural properties of biomolecules are dictated by their intrinsic conformational energetics in combination with environmental contributions. Calculations using high-level ab initio methods on the deoxyribonucleosides have been performed to investigate the influence of base on the intrinsic conformational energetics of nucleosides. Energy minima in the north and south ranges of the deoxyribose pseudorotation surfaces have been located, allowing characterization of the influence of base on the structures and energy differences between those minima. With all bases, chi values associated with the south energy minimum are lower than in canonical B-DNA, while chi values associated with the north energy minimum are close to those in canonical A-DNA. In deoxycytidine, chi adopts an A-DNA conformation in both the north and south energy minima. Energy differences between the A and B conformations of the nucleosides are <0.5 kcal/mol in the present calculations, except with deoxycytidine, where the A form is favored by 2.3 kcal/mol, leading the intrinsic conformational energetics of GC basepairs to favor the A form of DNA by 1.5 kcal/mol as compared with AT pairs. This indicates that the intrinsic conformational properties of cytosine at the nucleoside level contribute to the A form of DNA containing predominately GC-rich sequences. In the context of a B versus Z DNA equilibrium, deoxycytidine favors the Z form over the B form by 1.6 kcal/mol as compared with deoxythymidine, suggesting that the intrinsic conformational properties of cytosine also contribute to GC-rich sequences occurring in Z DNA with a higher frequency than AT-rich sequences. Results show that the east pseudorotation energy barrier involves a decrease in the furanose amplitude and is systematically lower than the inversion barrier, with the energy differences influenced by the base. Energy barriers going from the south (B form) sugar pucker to the east pseudorotation barrier are lower in pyrimidines as compared with purines, indicating that the intrinsic conformational properties associated with base may also influence the sugar pseudorotational population distribution seen in DNA crystal structures and the kinetics of B to A transitions. The present work provides evidence that base composition, in addition to base sequence, can influence DNA conformation.

Modeling high-resolution hydration patterns in correlation with DNA sequence and conformation

Hydration around the DNA fragment d(C5T5).(A5G5) is presented from two molecular dynamics simulations of 10 and 12 ns total simulation time. The DNA has been simulated as a flexible molecule with both the CHARMM and AMBER force fields in explicit solvent including counterions and 0.8 M additional NaCl salt. From the previous analysis of the DNA structure B-DNA conformations were found with the AMBER force-field and A-DNA conformations with CHARMM parameters. High-resolution hydration patterns are compared between the two conformations and between C.G and T.A base-pairs from the homopolymeric parts of the simulated sequence. Crystallographic results from a statistical analysis of hydration sites around DNA crystal structures compare very well with the simulation results. Differences between the crystal sites and our data are explained by variations in conformation, sequence, and limitations in the resolution of water sites by crystal diffraction. Hydration layers are defined from radial distribution functions and compared with experimental results. Excellent agreement is found when the measured experimental quantities are compared with the equivalent distribution of water molecules in the first hydration shell. The number of water molecules bound to DNA was found smaller around T.A base-pairs and around A-DNA as compared to B-DNA. This is partially offset by a larger number of water molecules in hydrophobic contact with DNA around T.A base-pairs and around A-DNA. The numbers of water molecules in minor and major grooves have been correlated with helical roll, twist, and inclination angles. The data more fully explain the observed B-->A transition at low humidity.

A modified version of the Cornell et al. force field with improved sugar pucker phases and helical repeat

We have examined some subtle parameter modifications to the Cornell et al. force field, which has proven quite successful in reproducing nucleic acid properties, but whose C2'-endo sugar pucker phase and helical repeat for B DNA appear to be somewhat underestimated. Encouragingly, the addition of a single V2 term involving the atoms C(sp3)-O-(sp3)-C(sp3)-N(sp2), which can be nicely rationalized because of the anomeric effect (lone pairs on oxygen are preferentially oriented relative to the electron withdrawing N), brings the sugar pucker phase of C2'-endo sugars to near perfect agreement with ab initio calculations (W near 162 degrees). Secondly, the use of high level ab initio calculations on entire nucleosides (in contrast to smaller model systems necessitated in 1994-95 by computer limitations) lets one improve the chi torsional potential for nucleic acids. Finally, the O(sp3)-C(sp3)- C(sp3)-O(sp3) V2 torsional potential has been empirically adjusted to reproduce the ab initio calculated relative energy of C2'-endo and C3'-endo nucleosides. These modifications are tested in molecular dynamics simulations of mononucleosides (to assess sugar pucker percentages) and double helices of DNA and RNA (to assess helical and sequence specific structural properties). In both areas, the modified force field leads to improved agreement with experimental data.

Molecular dynamics and continuum solvent studies of the stability of polyG-polyC and polyA-polyT DNA duplexes in solution

Molecular dynamics simulation in explicit solvent and continuum solvent models are applied to investigate the relative stability of A- and B-form helices for two DNA sequences, dA10-dT10 and dG10-dC10 in three structural forms. One structural form is based on an unrestrained molecular dynamics (MD) trajectory starting from a canonical B-DNA structure, the second is based on a MD trajectory starting in a canonical B-DNA structure with the sugars constrained to be C2'-endo and the third simulation started from a canonical A-DNA structure with the sugars constrained to C3'-endo puckers. For the energetic analysis, structures were taken as snapshots from nanosecond length molecular dynamics simulations computed in a consistent fashion in explicit solvent, applying the particle mesh Ewald method and the Cornell et al. force field. The electrostatic contributions to solvation free energies are computed using both a finite-difference Poisson-Boltzmann model and a pairwise Generalized Born model. The non-electrostatic contributions to the solvation free energies are estimated with a solvent accessible surface area dependent term. To estimate the gas phase component of the relative free energy between the various structures, the mean solute internal energies (determined with the Cornell et al. molecular mechanics potential including all pairwise interactions within the solute) and estimates of the solute entropy (using a harmonic approximation) were used. Consistent with experiment, the polyG-polyC (GC) structures are found to be much more A-phillic than the polyA-polyT (AT) structures, the latter being quite A-phobic. The dominant energy components responsible for this difference comes from the internal and van der Waal energies. A perhaps less appreciated difference between the GC and AT rich sequences is suggested by the calculated salt dependence which demonstrates a significantly enhanced ability to drive GC rich sequences towards an A-form structure compared to AT rich sequences. In addition to being A-phobic, the AT structure also has a noticably larger helical repeat than GC and other mixed sequence duplexes, consistent with experiment. Analysis of the average solvent density from the trajectories shows hydration patterns in qualitative agreement with experiment and previous theoretical treatments.