Molecular dynamics anneals large-scale deformations of model macromolecules: stretching the DNA double helix to form an intercalation site

Theoretical studies of the intercalation of 9-hydroxyellipticine in DNA

Extensive molecular dynamics (MD) simulations have been used to investigate the intercalative binding of 9-hydroxyellipticine to the DNA oligonucleotide d(ATATATATATAT)2. Four independent simulations differing in the initial orientation of the drug at the intercalation site were carried out, and compared both with each other and a control simulation of the free DNA sequence. The structure of the latter was compared with structures obtained from x-ray crystallography and nmr spectroscopy, as well as the theoretically derived "alternating B-DNA" model [A. Klug et al. (1979), Journal of Molecular Biology, Vol. 131, p. 669]. The alternation of twist angles observed in experimental structures was reproduced in the simulation. All four independent simulations of the drug-DNA intercalation complex converged in placing the pyridine ring of the ellipticine chromophore in the major groove; in one case this involved a 180 degrees rotation of the drug at the intercalation site. At a more detailed level, the drug is seen to be capable of adopting several distinct orientations, each stable over a period of hundreds of pico-seconds. Despite the presence of several polar groups in the drug, however, no direct hydrogen bonding to the DNA occurs; instead, interactions between the methyl groups of the drug and the thymine bases at the intercalation site appear important in determining the orientational preferences of the drug. Comparison of the intercalation complexes with the free DNA sequence shows a degree of unwinding resulting from intercalation, in good agreement with experimental results, but spread over the three central base-pair steps, not confined to the intercalation site itself. Measurements of torsional rigidity indicate only a slight stiffening of the DNA restricted to the immediate site of intercalation. The structures obtained from the MD simulations were used to calculate theoretical CD spectra, with separate simulations giving very different results. This appears to indicate that given an accurate assignment of the main electronic transition dipole moment of the ellipticine chromophore, discrimination of the more realistic binding geometries may be possible. The relative merits of the various drug orientations observed in the simulations are discussed and a perpendicular orientation of the drug at the intercalation site is considered to be the most consistent with experimental data. While the simulations themselves represent a total of over 2 ns, however, the differences apparent between independent runs indicate that longer simulation times will be required before a complete, unequivocal view of DNA intercalation is obtained.

Conformational transitions using molecular dynamics with minimum biasing

The molecular dynamics algorithm (MD), which simulates intramolecular motions on the subnanosecond timescale, has been modified to allow the investigation of slow conformational transitions that do not necessarily occur spontaneously in MD simulations. The method is designated CONTRA MD (CONformational TRAnsitions by Molecular Dynamics with minimum biasing). The method requires the prior definition of a single conformational variable that is required to vary monotonically from an initial conformation to a final target conformation. The simulation is broken up into a series of short free MD segments, and we determine, after each segment of MD, whether or not the system has evolved toward the final conformation. Those segments that do not move the system in that direction are deleted. Those that do move it toward the final conformation are patched together sequentially to generate a single representative trajectory along the transition pathway. The CONTRA MD method is demonstrated first by application to the simultaneous C2'-endo to C3'-endo repucker and anti to syn N-glycosidic torsion transitions in 2'-deoxyadenosine and then to the large-scale bending in phenylalanine transfer RNA.

Binding site for ethidium cation in the major groove of B-form DNA

Molecular modeling of the system composed of ethidium cation initially intercalated through the major and minor grooves of the B-DNA form of 5'GCATGC3' into the central AT pairs, with the phenyl group oriented either toward or away from the helical axis, led upon energy minimization to intercalation complexes only when the phenyl group was initially oriented away from the helical axis. For the other two cases, energy minimization led to extrusion of the ethidium from the helix to form unanticipated outside-bound complexes stabilized by specific hydrogen bonds. It is suggested that outside-bound major groove complexes involving the GXXXG sequence may play important roles in the reaction mechanism of ethidium intercalation and in its action as a drug.

Conformation and dynamics of drug-DNA intercalation

Molecular dynamics simulations have been undertaken for a B-form dodecanucleotide duplex in solution with and without an intercalated proflavine molecule between the central C.G base pairs. The introduction of this simple intercalator affects both the conformational features and dynamic properties of the oligonucleotide double helix. Changes are seen in the rms atomic fluctuations and anisotropy of phosphate, sugar and base atoms. The backbone conformation is slightly changed on average and more sugars adopt the C3' endo conformation in the simulation of the complex compared with the simulation of the oligonucleotide alone. Both major and minor grooves becomes wider on average with the addition of the intercalating drug. Flanking A.T base pairs on both sides of the intercalation site have undergone an increase in flexibility, with the base pairs, especially at the 5' side, having the N1...N3 hydrogen bonds being broken.

Molecular dynamics simulations of dinucleoside and dinucleoside-drug crystal hydrates

Molecular dynamics simulations have been performed on the dinucleoside monophosphates rGpC and dCpG, the latter in its intercalation complex with the acridine drug proflavine. The simulations were performed on the crystal structures, with crystallographically-located solvent molecules. It was found that satisfactory results were best obtained with restraints placed on the movements of the water molecules. Motions of individual atoms have been examined in terms of rms fluctuations and anisotropy and correlation functions. Relative motions of groups (phosphates, sugars, bases and proflavine molecules) have been analysed.

A molecular dynamics study of the effect of G.T mispairs on the conformation of DNA in solution

The effect of G.T mispair incorporation into a double-helical environment was examined by molecular dynamics simulation. The 60-ps simulations performed on the two hexanucleotide duplexes d (G3C3)2 and d(G3TC2)2 included 10 Na+ counterions and first hydration shell waters. The resulting backbone torsional angle trajectories were analyzed to select time spans representative of conformational domains. The average backbone angles and helical parameters of the last time span for both duplexes are reported. During the simulation the hexamers retained B-type DNA structures that differed from typical A- or B-DNA forms. The overall helical structures for the two duplexes are vary similar. The presence of G.T mispairs did not alter the overall helical structure of the oligonucleotide duplex. Large propeller twist and buckle angles were obtained for both duplexes. The purine/pyrimidine crossover step showed a large decrease in propeller twist in the normal duplex but not in the mismatch duplex. Upon the formation of wobble mispairs in the mismatched duplex, the guanines moved into the minor groove and the thymines moved into the major groove. This helped prevent purine/purine clash and created a deformation in the relative orientation of the glycosidic bonds. It also exposed the free O4 of the thymines in the major groove and N2 of the guanines in the minor groove to interactions with solvent and counterions. These factors seemed to contribute to the apparently higher rigidity of the mismatched duplex during the simulation.

A molecular dynamics investigation of the elastomeric restoring force in elastin

A repetitive polypentapeptide organized as a connected chain of beta-bends is believed to be an important structural element of elastin, the major elastomer in biological systems. Molecular dynamics simulations were carried out on hydrated polymers of (Val-Pro-Gly-Val- Gly)18 at various extensions. Analysis of the fluctuations of backbone angles in relaxed elastin showed that particularly large-amplitude torsional motions occur in phi and psi angles of residues connecting sequentially adjacent hairpin bends. Many such motions reflect peptide plane librations that result from anticorrelated crankshaft rotations of psi i and phi i+1. These effects were much reduced in stretched polymer models. The conformational entropy of relaxed and stretched elastin models was estimated using a treatment due to Meirovitch, and gave a calculated decrease in entropy of about 1 cal/mol deg when the polymer was stretched to 1.75 times its original length. There are large changes in solvent-accessible surface area during the initial stages of elastin stretching. Collectively these results suggest that hydrophobic interactions make contributions to elastin entropy at low extensions, but that librational mechanisms make larger contributions to the elastic restoring force at longer extensions.

The electrostatic potential of B-DNA

Electrostatic potentials around DNA are obtained by solving the nonlinear Poisson-Boltzmann (PB) equation. The detailed charge distribution of the DNA and the different polarizabilities of the macromolecule and solvent are included explicitly in the calculations. The PB equation is solved using extensions of a finite difference approach applied previously to proteins. Electrical potentials and ion concentrations are compared to those obtained with simpler models. It is found that the shape of the dielectric boundary between the macromolecule and solvent has significant effects on the calculated potentials near the surface, particularly in the grooves. Sequence-specific patterns are found, the most surprising result being the existence of positive regions of potential near the bases in both the major and minor grooves. The effect of solvent and ionic atmosphere screening of phosphate-phosphate repulsions is studied, and an effective dielectric function, appropriate for molecular mechanics simulations, is derived.