Localization of Divalent Metal Ions in the Minor Groove of DNA A-Tracts

Assessment of the molecular dynamics structure of DNA in solution based on calculated and observed NMR NOESY volumes and dihedral angles from scalar coupling constants

To assess the accuracy of the molecular dynamics (MD) models of nucleic acids, a detailed comparison between MD-calculated and NMR-observed indices of the dynamical structure of DNA in solution has been carried out. The specific focus of our comparison is the oligonucleotide duplex, d(CGCGAATTCGCG)(2), for which considerable structural data have been obtained from crystallography and NMR spectroscopy. An MD model for the structure of d(CGCGAATTCGCG)(2) in solution, based on the AMBER force field, has been extended with a 14 ns trajectory. New NMR data for this sequence have been obtained in order to allow a detailed and critical comparison between the calculated and observed parameters. Observable two-dimensional (2D) nuclear Overhauser effect spectroscopy (NOESY) volumes and scalar coupling constants were back-calculated from the MD trajectory and compared with the corresponding NMR data. The comparison of these results indicate that the MD model is in generally good agreement with the NMR data, and shows closer accord with experiment than back-calculations based on the crystal structure of d(CGCGAATTCGCG)(2) or the canonical A or B forms of the sequence. The NMR parameters are not particularly sensitive to the known deficiency in the AMBER MD model, which is a tendency toward undertwisting of the double helix when the parm.94 force field is used. The MD results are also compared with a new determination of the solution structure of d(CGCGAATTCGCG)(2) using NMR dipolar coupling data.

Influence of netropsin's charges on the minor groove width of d(CGCGAATTCGCG)2

The exact understanding of the interaction of minor groove binding drugs with DNA is of interest due to their importance as transcription controlling drugs. In this study we performed four molecular dynamics simulations, one of the uncomplexed d(CGCGAATTCGCG)(2) dodecamer and three simulations of the DNA complexed with the minor groove binder netropsin. The charged guanidinium and amidinium ends of the small ligand were in one simulation formally uncharged, in the second one normally charged, and in the third simulation we doubled the charges of the two ends. So we are able to filter out the influence the charges exert on the DNA structure. The positive charges reduce the width of the minor groove showing that charges are able to modify the groove width by charge neutralization of the negative phosphate groups. The quality of the used force field was successfully tested by comparing the results of the uncomplexed dodecamer with already reported NMR and x-ray studies. Thus our simulations should be able to describe the minor groove width of DNA in a correct manner underlying the validity of the results.

Comparative bending dynamics in DNA with and without regularly repeated adenine tracts

The macroscopic curvature of double helical DNA induced by regularly repeated adenine tracts is well known but still puzzling. Its physical origin remains controversial even though it is perhaps the best-documented sequence modulation of DNA structure. The paper reports on comparative theoretical and experimental studies of bending dynamics in 35-mer DNA fragments. This length appears large enough for the curvature to be distinguished by gel electrophoresis. Two DNA fragments, with identical base pair composition but different sequences, are compared. In the first one, a single A-tract motif is four times repeated in phase with the helical screw whereas the second sequence is "random." Both calculations and experiments indicate that the A-tract DNA is distinguished by large static curvature and characteristic bending dynamics, suggesting that the computed effect corresponds to the experimental phenomenon. The results agree poorly with the view that DNA bending is caused by the specific local geometry of base pair stacking or binding of solvent counterions, but lend additional support to the hypothesis of a compressed frustrated state of the backbone as the principal physical cause of the static curvature. Possible ways of experimental verification of this hypothesis are discussed.

Molecular dynamics simulation of nucleic acids: successes, limitations, and promise

In the last five years we have witnessed a significant increase in the number publications describing accurate and reliable all-atom molecular dynamics simulations of nucleic acids. This increase has been facilitated by the development of fast and efficient methods for treating the long-range electrostatic interactions, the availability of faster parallel computers, and the development of well-validated empirical molecular mechanical force fields. With these technologies, it has been demonstrated that simulation is not only capable of consistently reproducing experimental observations of sequence specific fine structure of DNA, but also can give detailed insight into prevalent problems in nucleic acid structure, ion association and specific hydration of nucleic acids, polyadenine tract bending, and the subtle environmental dependence of the A-DNA-B-DNA duplex equilibrium. Despite the advances, there are still issues with the methods that need to be resolved through rigorous controlled testing. In general, these relate to deficiencies of the underlying molecular mechanical potentials or applied methods (such as the imposition of true periodicity in Ewald simulations and the need for energy conservation), and significant limits in effective conformational sampling. In this perspective, we provide an overview of our experiences, provide some cautionary notes, and provide recommendations for further study in molecular dynamics simulation of nucleic acids.

DNA-cation interactions: quo vadis?

The interactions between double helical DNA and cations, specifically mono- and divalent metal ions, have recently received increased attention. Molecular dynamics simulations, solution NMR, and X-ray crystallography have all shed light on the coordination of ions in the major and minor grooves of DNA. Metal ion interactions may play key roles in the control of DNA conformation and topology, but despite progress in locating the ions and determining their precise binding modes, it remains difficult to figure out just how important ions really are. What have we learned and what remains to be done?

Do water molecules mediate protein-DNA recognition?

A comprehensive analysis of interfacial water molecules in the structures of 109 unique protein-DNA complexes is presented together with a new view on their role in protein-DNA recognition. Location of interfacial water molecules as reported in the crystal structures and as emerging from a series of molecular dynamics studies on protein-DNA complexes with explicit solvent and counterions, was analyzed based on their acceptor, donor hydrogen bond relationships with the atoms and residues of the macromolecules, electrostatic field calculations and packing density considerations. Water molecules for the purpose of this study have been categorized into four classes: viz. (I) those that contact both the protein and the DNA simultaneously and thus mediate recognition directly; (II) those that contact either the protein or the DNA exclusively via hydrogen bonds solvating each solute separately; (III) those that contact the hydrophobic groups in either the protein or the DNA; and, lastly (IV) those that contact another water molecule. Of the 17,963 crystallographic water molecules under examination, about 6% belong to class I and 76% belong to class II. About three-fourths of class I and class II water molecules are exclusively associated with hydrogen bond acceptor atoms of both protein and DNA. Noting that DNA is polyanionic, it is significant that a majority of the crystallographically observed water molecules as well as those from molecular dynamics simulations should be involved in facilitating binding by screening unfavorable electrostatics. Less than 2% of the reported water molecules occur between hydrogen bond donor atoms of protein and acceptor atoms of DNA. These represent cases where protein atoms cannot reach out to DNA to make favorable hydrogen bond interactions due to packing/structural restrictions and interfacial water molecules provide an extension to side-chains to accomplish hydrogen bonding.

Molecular dynamics simulations of B '-DNA: sequence effects on A-tract-induced bending and flexibility

Molecular dynamics (MD) simulations including water and counterions are reported on five examples of A-tract DNA oligonucleotide dodecamer duplexes for which crystal structures are available, the homopolymeric duplex sequences poly(dA) and poly(dG), and two related sequences that serve as controls. MD was performed using the AMBER suite of programs for 3 ns on each sequence. These results, combined with previously reported MDs on 25-mer and 30-mer oligonucleotides on sequences with phased A-tracts carried out under a similar simulation protocol, are used to examine salient issues in the structural chemistry of ApA steps and A-tract induced axis bending. MD modeling successfully describes the distinctive B' structure of A-tracts in solution as essentially straight (wedge angles of <1 degrees ), more rigid than generic B-form DNA, with slight base-pair inclination, high propeller twist and a minor groove narrowing 5' to 3'. The MD structures in solution agree closely with corresponding crystal structures, supporting the idea that crystal structures provide a good model for A-tract DNA structure in solution. From the collective MD results, bending and flexibility are calculated by step. Pyrimidine-purine steps are predicted to be most intrinsically bent and also most bendable, i.e. susceptible to bending. Pyrimidine-pyrimidine ( approximately purine-purine) and purine-pyrimidine steps show less intrinsic deformation and deformability. The MD calculated flexibility correlates well with the protein-induced bendability derived independently from the protein DNA crystal structures. The MD results indicate that bending and flexibility of base-pair steps in DNA are highly correlated, i.e. steps that exhibit the most intrinsic deformation from B-form DNA turn are also the most dynamically deformable. The MD description of A-tract-induced axis bending shows most consistency with the non A-tract, general-sequence model, in which the sequence curvature originates primarily in base-pair roll towards the major groove in non-A-tract regions of the sequence, particularly pyrimidine-purine steps. The direction of curvature is towards the minor groove viewed from opposite the A-tracts, but the A-tracts per se exhibit only minor deformation. The MD results are found to be consistent with the directionality of bending inferred for DNA sequences from gel retardation and cyclization experiments.

Localization of Fe(2+) at an RTGR sequence within a DNA duplex explains preferential cleavage by Fe(2+) and H2O2

Nicking of duplex DNA by the iron-mediated Fenton reaction occurs preferentially at a limited number of sequences. Of these, purine-T-G-purine (RTGR) is of particular interest because it is a required element in the upstream regulatory regions of many genes involved in iron and oxidative-stress responses. In order to study the basis of this preferential nicking, NMR studies were undertaken on the RTGR-containing duplex oligonucleotide, d(CGCGATATGACACTAG)/d(CTAGTGTCATATCGCG). One-dimensional and two-dimensional 1H NMR measurements show that Fe(2+) interacts preferentially and reversibly at the ATGA site within the duplex at a rate that is rapid relative to the chemical-shift timescale, while selective paramagnetic NMR line-broadening of the ATGA guanine H8 suggests that Fe(2+) interacts with the guanine N7 moiety. Localization at this site is supported by Fe(2+) titrations of a duplex containing a 7-deazaguanine substitution in place of the guanine in the ATGA sequence. The addition of a 100-fold excess of Mg(2+) over Fe(2+) does not affect the Fe(2+)-dependent broadening. When the ATGA site in the duplex is replaced by ATGT, an RTGR site (GTGA) is created on the opposite strand. Preferential iron localization then takes place at the 3' guanine in GTGA but no longer at the guanine in ATGT, consistent with the lack of preferential cleavage of ATGT sites relative to ATGA sites.

DNA bending by asymmetrically tethered cations: influence of tether flexibility

BACKGROUND

We have been studying the proposal that laterally asymmetric charge neutralization along the DNA double helix can induce collapse toward the neutralized surface. Results of previous experiments implied that such a phenomenon can occur, suggesting a role for local interphosphate repulsive forces in DNA shape and rigidity.

RESULTS

We now show that, whereas six ammonium ions tethered to one DNA face on flexible propyl chains can induce detectable DNA curvature, tethering of ammonium ions on rigid propynyl tethers does not induce DNA curvature. Molecular modeling indicates differing propensities for phosphate salt bridge formation between propyl- and propynyl-tethered ammonium ions.

CONCLUSIONS

Ammonium ion localization is suggested as a key factor in induced bending. Rigidification of the double helix by stacking of propyne groups cannot be excluded.

Significance of ligand tails for interaction with the minor groove of B-DNA

Minor groove binding ligands are of great interest due to their extraordinary importance as transcription controlling drugs. We performed three molecular dynamics simulations of the unbound d(CGCGAATTCGCG)(2) dodecamer and its complexes with Hoechst33258 and Netropsin. The structural behavior of the piperazine tail of Hoechst33258, which has already been shown to be a contributor in sequence-specific recognition, was analyzed. The simulations also reveal that the tails of the ligands are able to influence the width of the minor groove. The groove width is even sensitive for conformational transitions of these tails, indicating a high adaptability of the minor groove. Furthermore, the ligands also exert an influence on the B(I)/B(II) backbone conformational substate behavior. All together these results are important for the understanding of the binding process of sequence-specific ligands.

DNA-cation interactions: The major and minor grooves are flexible ionophores

Several crystallographic, solution-state and theoretical studies carried out this past year provide new support for the sequence-specific nature of monovalent and divalent cation coordination within the DNA major and minor grooves. Correlations observed between groove width and cation coordination indicate that the grooves are flexible and respond to cation binding.

Changes in 13C NMR chemical shifts of DNA as a tool for monitoring drug interactions

The antibiotic drug, netropsin, was complexed with the DNA oligonucleotide duplex [d(GGTATACC)]2 to explore the effects of ligand binding on the 13C NMR chemical shifts of the DNA base and sugar carbons. The binding mode of netrospin to TA-rich tracts of DNA has been well documented and served as an attractive model system. For the base carbons, four large changes in resonance chemical shifts were observed upon complex formation: -0.64 ppm for carbon 4 of either Ado4 or Ado6, 1.36 ppm for carbon 2 of Thd5, 1.33 ppm for carbon 5 of Thd5 and 0.94 for carbon 6 of Thd5. AdoC4 is covalently bonded to a heteroatom that is hydrogen bonded to netropsin; this relatively large deshielding is consistent with the known hydrogen bond formed at AdoN3. The three large shielding increases are consistent with hydrogen bonds to water in the minor groove being disrupted upon netropsin binding. For the DNA sugar resonances, large changes in chemical shifts were observed upon netropsin complexation. The 2', 3' and 5' 13C resonances of Thd3 and Thd5 were shielded whereas those of Ado4 and Ado6 were deshielded; the 13C resonances of 1' and 4' could not be assigned. These changes are consistent with alteration of the dynamic pseudorotational states occupied by the DNA sugars. A significant alteration in the pseudorotational states of Ado4 or Ado6 must occur as suggested by the large change in chemical shift of -1.65 ppm of the C3' carbon. In conclusion, 13C NMR may serve as a practical tool for analyzing structural changes in DNA-ligand complexes.

Macrochelation, cyclometallation and G-quartet formation: N3- and C8-bound PdII complexes of adenine and guanine

The reactions of Pd(II) ions with a series of chelate-tethered derivatives of adenine and guanine have been studied and reveal a difference in the reactivity of the purine bases. Reactions of [PdCl2(MeCN)2] and A-alkyl-enH x Cl (alkyl = propyl or ethyl, A adenine, en = ethylenediamine) yield the monocationic species [PdCl(A-N3-Et-en)]+ (1) and [PdCl(A-N3-Pr-en)]+ (2). Both involve co-ordination at the minor groove site N3 of the nucleobase as confirmed by single-crystal X-ray analysis. Reactions with the analogous G-alkyl-enH x Cl derivatives (G=guanine, alkyl = ethyl or propyl) were more complex with a mixture of species being observed. For G-Et-en HCI a product was isolated which was identified as [PdCl(G-C8-Et-en)]+ (3). This compound contains a biomolecular metal-carbon bond involving C8 of the purine base. Crystallography of a product obtained from reaction of G-Pr-enH x Cl and [Pd(MeCN)4][NO3]2 reveals an octacationic tetrameric complex (4), in which each ligand acts to bridge two metal ions through a combination of a tridentate binding mode involving the diamine and N3 and monodentate coordination at N7.

Electrostatic mechanisms of DNA deformation

The genomes of higher cells consist of double-helical DNA, a densely charged polyelectrolyte of immense length. The intrinsic physical properties of DNA, as well as the properties of its complexes with proteins and ions, are therefore of fundamental interest in understanding the functions of DNA as an informational macromolecule. Because individual DNA molecules often exceed 1 cm in length, it is clear that DNA bending, folding, and interaction with nuclear proteins are necessary for packaging genomes in small volumes and for integrating the nucleotide sequence information that guides genetic readout. This review first focuses on recent experiments exploring how the shape of the densely charged DNA polymer and asymmetries in its surrounding counterion distribution mutually influence one another. Attention is then turned to experiments seeking to discover the degree to which asymmetric phosphate neutralization can lead to DNA bending in protein-DNA complexes. It is argued that electrostatic effects play crucial roles in the intrinsic, sequence-dependent shape of DNA and in DNA shapes induced by protein binding.

Molecular dynamics simulation of nucleic acids

We review molecular dynamics simulations of nucleic acids, including those completed from 1995 to 2000, with a focus on the applications and results rather than the methods. After the introduction, which discusses recent advances in the simulation of nucleic acids in solution, we describe force fields for nucleic acids and then provide a detailed summary of the published literature. We emphasize simulations of small nucleic acids ( approximately 6 to 24 mer) in explicit solvent with counterions, using reliable force fields and modern simulation protocols that properly represent the long-range electrostatic interactions. We also provide some limited discussion of simulation in the absence of explicit solvent. Absent from this discussion are results from simulations of protein-nucleic acid complexes and modified DNA analogs. Highlights from the molecular dynamics simulation are the spontaneous observation of A B transitions in duplex DNA in response to the environment, specific ion binding and hydration, and reliable representation of protein-nucleic acid interactions. We close by examining major issues and the future promise for these methods.

DNA structure: what's in charge?

DNA structure is well known to be sensitive to hydration and ionic strength. Recent theoretical predictions and experimental observations have raised the idea of the intrusion of monovalent cations into the minor groove spine of hydration in B-form DNA. To investigate this further, extensions and further analysis of molecular dynamics (MD) simulations on d(CGCCGAATTCGCG), d(ATAGGCAAAAAATAGGCAAAAATGG) and d(G(5)-(GA(4)T(4)C)(2)-C(5)), including counterions and water, have been performed. To examine the effective of minor groove ions on structure, we analyzed the MD snapshots from a 15 ns trajectory on d(CGCGAATTCGCG) as two subsets: those exhibiting a minor groove water spine and those with groove-bound ions. The results indicate that Na(+) at the ApT step of the minor groove of d(CGCCGAATTCGCG) makes only small local changes in the DNA structure, and these changes are well within the thermal fluctuations calculated from the MD. To examine the effect of ions on the differential stability of a B-form helix, further analysis was performed on two longer oligonucleotides, which exhibit A-tract-induced axis bending localized around the CpG step in the major groove. Plots of axis bending and proximity of ions to the bending locus were generated as a function of time and revealed a strong linear correlation, supporting the idea that mobile cations play a key role in local helix deformations of DNA and indicating ion proximity just precedes the bending event. To address the issue of "what's in charge?" of DNA structure more generally, the relative free energy of A and B-form d(CGCGAATTCGCG) structures from MD simulations under various environmental circumstances were estimated using the free energy component method. The results indicate that the dominant effects on conformational stability come from the electrostatic free energy, but not exclusively from groove bound ions per se, but from a balance of competing factors in the electrostatic free energy, including phosphate repulsions internal to the DNA, the electrostatic component of hydration (i.e. solvent polarization), and electrostatic effects of the counterion atmosphere. In summary, free energy calculations indicate that the electrostatic component is dominant, MD shows temporal proximity of mobile counterions to be correlated with A-track-induced bending, and thus the mobile ion component of electrostatics is a significant contributor. However, the MD structure of the dodecamer d(CGCGAATTCGCG) is not highly sensitive to whether there is a sodium ion in the minor groove.

A-Tract bending: insights into experimental structures by computational models

While solution structures of adenine tract (A-tract) oligomers have indicated a unique bend direction equivalent to negative global roll (commonly termed "minor-groove bending"), crystallographic data have not unambiguously characterized the bend direction; nevertheless, many features are shared by all A-tract crystal and solution structures (e.g. propeller twisting, narrow minor grooves, and localized water spines). To examine the origin of bending and to relate findings to the crystallographic and solution data, we analyze molecular dynamics trajectories of two solvated A-tract dodecamers: 1D89, d(CGCGA(6)CG), and 1D98, d(CGCA(6)GCG), using a new general global bending framework for analyzing bent DNA and DNA/protein complexes. It is significant that the crystallographically-based initial structures are converted from dissimilar to similar bend directions equivalent to negative global roll, with the average helical-axis bend ranging from 10.5 degrees to 14.1 degrees. The largest bend occurs as positive roll of 12 degrees on the 5' side of the A-tracts (supporting a junction model) and is reinforced by gradual curvature at each A-tract base-pair (bp) step (supporting a wedge model). The precise magnitude of the bend is subtly sequence dependent (consistent with a curved general sequence model). The conversion to negative global roll only requires small local changes at each bp, accumulated over flexible moieties both outside and inside the A-tract. In contrast, the control sequence 1BNA, d(CGCGA(2)TTCGCG), bends marginally (only 6.9 degrees ) with no preferred direction. The molecular features that stabilize the bend direction in the A-tract dodecamers include propeller twisting of AT base-pairs, puckering differences between A and T deoxyriboses, a narrow minor groove, and a stable water spine (that extends slightly beyond the A-tract, with lifetimes approaching 0.2 ns). The sugar conformations, in particular, are proposed as important factors that support bent DNA. It is significant that all these curvature-stabilizing features are also observed in the crystallographic structures, but yield overall different bending paths, largely due to the effects of sequences outside the A-tract. These results merge structural details reported for A-tract structures by experiment and theory and lead to structural and dynamic insights into sequence-dependent DNA flexibility, as highlighted by the effect of an A-tract variant of a TATA-box element on bending and flexibility required for TBP binding.

Intrinsic bending in GGCC tracts as probed by fluorescence resonance energy transfer

Double-stranded oligonucleotides containing the sequence 5'-GGCC-3' can be intrinsically bent, according to X-ray crystallography and gel electrophoresis mobility studies. We have performed fluorescence resonance energy transfer (FRET) experiments with dye-labeled oligonucleotides to further investigate the solution structure of this sequence. We find that 5'-GGCC-3'-containing oligonucleotides bring 5'-attached donor and acceptor dyes much closer together than a comparable "straight" sequence that contains 5'-GCGC-3'. The bend angle for the 5'-GGCC-3' sequence is estimated to be approximately 70 degrees, much larger than the crystallographically observed 23 degrees kink but in agreement with other FRET work. In contrast to gel electrophoresis studies, divalent metal ions do not promote increased kinking in 5'-GGCC-3' above background as judged by FRET. Thus, sequence-dependent structural effects in DNA may be a complicating feature of FRET experiments.

Cation-pi and amino-acceptor interactions between hydrated metal cations and DNA bases. A quantum-chemical view

Cation-pi interactions between cytosine and hexahydrated cations have been characterized using ab initio method with inclusion of electron correlation effects, assuming idealized and crystal geometries of the interacting species. Hydrated metal cations can interact with nucleobases in a cation-pi manner. The stabilization energy of such complexes would be large and comparable to the one for cation-pi complex with benzene. Further, polarized water molecules belonging to the hydration shell of the cation are capable to form a strong hydrogen bond interaction with the nitrogen lone electron pair of the amino groups of bases and enforce a pronounced sp3 pyramidalization of the nucleobase amino groups. However, in contrast to the benzene-cation complexes, the cation-pi configurations are highly unstable for a nucleobase since the conventional in plane binding of hydrated cations to the acceptor sites on the nucleobase is strongly preferred. Thus, a cation-pi interaction with a nucleobase can occur only if the position of the cation is locked above the nucleobase plane by another strong interaction. This indeed can occur in biopolymers and may have an effect on the local DNA architecture. Nevertheless, nucleobases have no intrinsic propensity to form cation-pi interactions.

An A-type double helix of DNA having B-type puckering of the deoxyribose rings

DNA usually adopts structure B in aqueous solution, while structure A is preferred in mixtures of trifluoroethanol (TFE) with water. However, the octamer d(CCCCGGGG) and other d(C(n)G(n)) fragments of DNA provide CD spectra that suggest that the base-pairs are stacked in an A-like fashion even in aqueous solution. Yet, d(CCCCGGGG) undergoes a cooperative TFE-induced transition into structure A, indicating that an important part of the aqueous duplex retains structure B. NMR spectroscopy shows that puckering of the deoxyribose rings is of the B-type. Hence, combination of the information provided by CD spectroscopy and NMR spectroscopy suggests an unprecedented double helix of DNA in which A-like base stacking is combined with B-type puckering of the deoxyribose rings. In order to determine whether this combination is possible, we used molecular dynamics to simulate the duplex of d(CCCCGGGG). Remarkably, the simulations, completely unrestrained by the experimental data, provided a very stable double helix of DNA, exhibiting just the intermediate B/A features described above. The double helix contained well-stacked guanine bases but almost unstacked cytosine bases. This generated a hole in the double helix center, which is a property characteristic for A-DNA, but absent from B-DNA. The minor groove was narrow at the double helix ends but wide at the central CG step where the Watson-Crick base-pairs were buckled in opposite directions. The base-pairs stacked tightly at the ends but stacking was loose in the duplex center. The present double helix, in which A-like base stacking is combined with B-type sugar puckering, is relevant to replication and transcription because both of these phenomena involve a local B-to-A transition.

Nucleic acids: theory and computer simulation, Y2K

Molecular dynamics simulations on DNA and RNA that include solvent are now being performed under realistic environmental conditions of water activity and salt. Improvements to force-fields and treatments of long-range interactions have significantly increased the reliability of simulations. New studies of sequence effects, axis bending, solvation and conformational transitions have appeared.

Sequence-specific binding of counterions to B-DNA

Recent studies by x-ray crystallography, NMR, and molecular simulations have suggested that monovalent counterions can penetrate deeply into the minor groove of B form DNA. Such groove-bound ions potentially could play an important role in AT-tract bending and groove narrowing, thereby modulating DNA function in vivo. To address this issue, we report here (23)Na magnetic relaxation dispersion measurements on oligonucleotides, including difference experiments with the groove-binding drug netropsin. The exquisite sensitivity of this method to ions in long-lived and intimate association with DNA allows us to detect sequence-specific sodium ion binding in the minor groove AT tract of three B-DNA dodecamers. The sodium ion occupancy is only a few percent, however, and therefore is not likely to contribute importantly to the ensemble of B-DNA structures. We also report results of ion competition experiments, indicating that potassium, rubidium, and cesium ions bind to the minor groove with similarly weak affinity as sodium ions, whereas ammonium ion binding is somewhat stronger. The present findings are discussed in the light of previous NMR and diffraction studies of sequence-specific counterion binding to DNA.

The hydration of nucleic acid duplexes as assessed by a combination of volumetric and structural techniques

Using high precision densimetric and ultrasonic measurements, we have determined, at 25 degrees C, the apparent molar volumes PhiV and the apparent molar compressibilities PhiK(S) of four nucleic acid duplexes-namely, the DNA duplex, poly(dIdC)poly(dIdC); the RNA duplex, poly(rA)poly(rU); and the two DNA/RNA hybrid duplexes, poly(rA)poly(dT) and poly(dA)poly(rU). Using available fiber diffraction data on these duplexes, we have calculated the molecular volumes as well as the solvent-accessible surface areas of the constituent charged, polar, and nonpolar atomic groups. We found that the hydration properties of these nucleic acid duplexes do not correlate with the extent and the chemical nature of the solvent-exposed surfaces, thereby suggesting a more specific set of duplex-water interactions beyond general solvation effects. A comparative analysis of our volumetric data on the four duplexes, in conjunction with available structural information, suggests the following features of duplex hydration: (a) The four duplexes exhibit different degrees of hydration, in the order poly(dIdC)poly(dIdC) > poly(dGdC)poly(dGdC) > poly(dAdT)poly(dAdT) approximately poly(dA)poly(dT). (b) Repetitive AT and IC sequences within a duplex are solvated beyond general effects by a spine of hydration in the minor groove, with this sequence-specific water network involving about 8 additional water molecules from the second and, perhaps, even the third hydration layers. (c) Repetitive GC and IC sequences within a duplex are solvated beyond general effects by a "patch of hydration" in the major groove, with this water network involving about 13 additional water molecules from the second and, perhaps, even the third hydration layers. (d) Random sequence, polymeric DNA duplexes, which statistically lack extended regions of repetitive AT, GC, or IC sequences, do not experience such specific enhancements of hydration. Consequently, consistent with our previous observations (T. V. Chalikian, A. P. Sarvazyan, G. E. Plum, and K. J. Breslauer, Biochemistry, 1994, Vol. 33, pp. 2394-2401), duplexes with approximately 50% AT content exhibit the weakest hydration, while an increase or decrease from this AT content causes enhancement of hydration, either due to stronger hydration of the minor groove (an increase in AT content) or due to stronger hydration of the major groove (an increase in GC content). (e) In dilute aqueous solutions, a B-DNA duplex is more hydrated than an A-DNA duplex, a volumetric-based conclusion that is in agreement with previous results obtained on crystals, fibers, and DNA solutions in organic solvent-water mixtures. (f) the A-like, RNA duplex poly(rA)poly(rU) and the structurally similar A-like, hybrid duplex poly(rA)poly(dT), exhibit similar hydration properties, while the structurally distinct A-like, hybrid duplex poly(rA)poly(dT) and non-A-like, hybrid duplex poly(dA)poly(rU) exhibit differential hydration properties, consistent with structural features dictating hydration characteristics. We discuss how volumetric characterizations, in conjunction with structural studies, can be used to describe, define, and resolve the general and sequence/conformation-specific hydration properties of nucleic acid duplexes.

Water and ions in a high resolution structure of B-DNA

A detailed picture of hydration and counterion location in the B-DNA duplex d(GCGAATTCG) is presented. Detailed data have been obtained by single crystal x-ray diffraction at atomic resolution (0.89 A) in the presence of Mg(2+). The latter is the highest resolution ever obtained for a B-DNA oligonucleotide. Minor groove hydration is compared with that found in the Na(+) and Ca(2+) crystal forms of the related dodecamer d(CGCGAATTCGCG). High resolution data (1.45 A) of the Ca(2+) form obtained in our laboratory are used for that purpose. The central GAATTC has a very stable hydration spine identical in all cases, independent of duplex length and crystallization conditions (counterions, space group). However, the organization of the water molecules (tertiary and quaternary layers) associated with the central spine vary in each case.

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.

Localization of ammonium ions in the minor groove of DNA duplexes in solution and the origin of DNA A-tract bending

Monovalent cation binding sites on nucleic acids in solution can be localized using the isotopically labeled ammonium ion (15NH4+) as a probe in high resolution NMR spectroscopy experiments. The application of this technique to a series of DNA duplexes reveals a preference for the binding of ammonium cations in the minor groove of A-tract sequences. These results are consistent with a recent report which indicates that some solvent electron densities previously identified as water molecules in DNA X-ray crystal structures are partially occupied by sodium ions. The sequence-specific nature of monovalent cation binding sites demonstrated here for A-tract DNA provides an explanation for the origin of sequence-directed bending.

Molecular dynamics simulations of an oligonucleotide duplex with adenine tracts phased by a full helix turn

A theoretical model of a DNA oligonucleotide duplex featuring A-tracts phased by a full helix turn is developed based on molecular dynamics computer simulation. The extent to which this model agrees with relevant experimental data on axis bending and the relationship of A-tracts to bending and other aspects of helix morphology is investigated. Specifically, a series of nanosecond-level molecular dynamics (MD) simulations have been carried out for the 25 bp duplex d(ATAGGCAAAAAATAGGCAAAAATGG) at various concentrations of saline solution. A 30 base-pair sequence composed of three 10 bp repeats of the BamHI recognition sequence ligated together, d(CGGGATCCCG. CGGGATCCCG.CGGGATCCCG), was simulated as a control. The MD was carried out using the AMBER 4.1 suite of programs, and utilized the Cornell et al. force-field with the electrostatic boundary conditions treated by the particle-mesh Ewald summation protocol. The MD results show that at a concentration of 60 mM KCl, 10 mM MgCl2 added salt plus minimal neutralizing cations, the MD model exhibits concerted axis bending to the extent of 15.5 degrees per A-tract. This compares favorably with the bending per turn of 17 to 21 degrees inferred from cyclization experiments. The MD model also exhibits a progressive 5' to 3' narrowing of the minor-groove region of A-tracts, a feature inferred from DNA footprinting experiments. Analysis of the dynamic structure of the MD models shows that the origin of the bending follows a junction-type bending model with an admixture of mixed sequence effects, with A-tracts relatively straight, as in oligonucleotide crystal structures of sequences containing A-tracts. The results are shown to be sensitive to environmental conditions: MD on d(ATAGGCAAAAAATAGGCAAAAATGG) in neutralizing Na+ buffer results in markedly reduced curvature, and the removal of Mg2+ measurably affects bending. Carrying out the simulations at experimental salt conditions appears to be essential to obtain an accurate account of the experimentally observed bending.

Insight into the stabilization of A-DNA by specific ion association: spontaneous B-DNA to A-DNA transitions observed in molecular dynamics simulations of d[ACCCGCGGGT]2 in the presence of hexaamminecobalt(III)

BACKGROUND

Duplex DNA is more than a simple information carrier. The sequence-dependent structure and its inherent deformability, in concert with the subtle modulating effects of the environment, play a crucial role in the regulation and packaging of DNA. Recent advances in force field and simulation methodologies allow molecular dynamics simulations to now represent the specific effects of the environment. An understanding of the environmental dependence of DNA structure gives insight into how histones are able to package DNA, how various proteins are able to bind and modulate nucleic acid structure and will ultimately aid the design of molecules to package DNA for more effective gene therapy.

RESULTS

Molecular dynamics simulations of d[ACCCGCGGGT]2 in solution in the presence of hexaamminecobalt(III) [Co(NH3)6(3+)] show stabilization of A-DNA and spontaneous B-DNA to A-DNA transitions, which is consistent with experimental results from NMR and Raman spectroscopic and X-ray crystallographic studies. In the absence of Co(NH3)6(3+), A-DNA to B-DNA transitions are observed instead. In addition to their interaction with the guanines in the major groove, Co(NH3)6(3+) ions bridge opposing strands in the bend across the major groove, probably stabilizing A-DNA.

CONCLUSIONS

The simulation methods and force fields have advanced to a sufficient level that some representation of the environment can be seen in nanosecond length molecular dynamics simulations. These simulations suggest that, in addition to the general explanation of A-DNA stabilization by dehydration, hydration and ion association in the major groove stabilize A-DNA.