Theoretical study of the hypochromic effect in polynucleotides]

The first UV-absorption band hypochromicity of poly(dA)-poly(dT), poly(dG)-poly(dC), poly(dA), poly(dT), poly(dG), poly(dC), is calculated with the help of the perturbation theory. The wave functions of the bases are computed by Pariser--Parr--Pople's method taking into account all the singly excited configurations. The results obtained show a good correlation between the theoretical and experimental values of hypochromicity. A considerable influence of the vaccum electron transitions on the hypochromicity of polynucleotides is revealed. The origin of the hypochromic effect in the double-stranded polynucleotides is investigated. It is shown that intrastrand interactions between the bases make the main contribution to hypochromicity (60-76%), while the contribution of the Watson-Crick pairs is small (2-12%). The essential part of hypochromicity (22-28%) is due to the interstrand interactions between the bases which are not coupled by hydrogen bonds. The discussion of the experimental data shows that the present theoretical investigation could serve as a basis for correct treatment of experimental results.     

Differences in melting behavior between homopolymers and copolymers of DNA: Role of nonbonded forces for GC and the role of the hydration spine and premelting transition for AT

Melting measurements of the mono-base-pair DNA polymers showed that the melting temperature T_m of the B-DNA homopolymer poly (dA ) · poly (dT) is higher than that of the copolymer poly [d(A-T)]. On the other hand, the T_mof the B-DNA homopolymer poly (dG) · poly (dC) is lower than that of the copolymer poly [d (G-C)]. From a structural point of view, the cross-strand base-stacking interaction in a DNA homopolymer is weaker than that in a DNA copolymer with the same base pair. One would then expect that all the DNA homopolymers are less stable than the copolymer with the same base pair. We find that the inversion of the melting order seen in the AT mono-base-pair DNA polymers is caused by the enhanced thermal stability of poly (dA) · poly (dT) from a well-defined spine of hydration attached to its minor groove. In this paper we employ the modified self-consistent phonon theory to calculate base-pair opening probabilities of four B-DNA polymers: poly(dA)-poly(dT), poly(dG) · poly(dC), poly[d(A-T)], and poly[d(G-C)] at temperatures from room temperature through the melting regions. Our calculations show that the spine of hydration can give the inverted melting order of the AT polymers as compared to the GC polymers in fair agreement with experimental measurements. Our calculated hydration spine disruption behavior in poly(dA) · poly(dT) at premelting temperatures is also in agreement with experimentally observed premelting transitions in poly (dA) · poly (dT). The work is in a sense a test of the validity of our models of nonbonded interactions and spine of hydration interactions. We find we have to develop the concept of a strained bond to fit observations in poly (dA) · poly(dT). The strained-bond concept also explains the otherwise anomalous stability of the hydration chain. © 1993 John Wiley & Sons, Inc.     

Binding of ligands to a one-dimensional heterogeneous lattice. III. Kinetic model and relaxation study of the interaction of tilorone with DNA and polynucleotides

A temperature-jump relaxation study of the interaction of tilorone with different polynucleotides and DNA has been performed. A single relaxation time, attributed to the intercalation step, has been observed in the case of poly[d(A-T)]·poly[d(A-T)], poly[d(A-C)]·poly[d(G-T)], poly[d(G-C)]·poly[d(G-C)], and poly(dG)·poly(dC). No intercalation into poly(dA)·poly(dT) occurs, and the interaction with poly(dG)·poly(dC) is different from what is observed with the other intercalating homopolymers. Refinement of the binding model is suggested from the analysis of the kinetic data. The relaxation curves obtained with DNA are well simulated based on a binding mechanism where DNA is considered a heterogeneous lattice and each type of site behaves as if it were located in the corresponding homopolymer. Poly(dA)·poly(dT) shows a unique behavior: studies of the effects of concentration and temperature indicate that tilorone acts as a probe of a process involving the polynucleotide alone. This process appears to be related to the dynamic structure of the nucleic acid and is detectable only when the bound dye is not intercalated.     

Conformational Peculiarities of Polynucleotides with a Nonrandom Base Sequence According to the 1H→ 3H Exchange Rate in C8H Groups of Purinic Residues

Abstract

We have determined the ¹H→³H exchange rate constants between water and C8H groups of purinic residues of alternating polynucleotides poly(dA-dT)·poly(dA-dT), poly(dG-dC)·poly(dG- dC) and poly(dA-dC)·poly(dG-dT) as well as homopolynucleotides poly(dA)·poly(dT) and poly(dG)·poly(dC) in aqueous solutions with high-salt concentrations (3 M NaCl and 4–6 M CsF), in water-ethanol (60%) solution and in 0.15 M NaCl at 25°C. The rate constants for adenine (k_A) and guanine (k_G) of polynucleotides were compared with corresponding constants for E.coli DNA, dGMP nd dAMP at the same conditions. The relation between exchange rates and conformations of polynucleotides permits the study of their conformational peculiarities in solution.

Of three alternating polynucleotides examined in 0.15 M NaCl the exchange retardation was observed only for poly(dA-dT)·poly(dA-dT) as compared with that in B-DNA, which is in good agreement with the B-alternating “wrinkled” DNA model. The conformations of poly(dG-dC)·poly(dG-dC) and poly(dA-dC)·poly(dG-dT), according to the exchange data obtained, are within the B form. For homopolynucleotides in 0.15 M NaCl, the k_A value for poly(dA)·poly(dT) is nearly the same as k_A for B-DNA, which indicates the similarity of their conformations, whereas the k_G value for poly(dG)·poly(dC) is 1.7-fold lower in comparison with the k_G value in B-DNA. This seems to be connected with the existence of B? A conformation equilibrium for poly(dG)·poly(dC) in solution.

The increase of NaCl concentration to 3 M results in a B→Z transition in the case of poly(dG-dC)·poly(dG-dC) and in the shift of B?A equilibrium towards the A-form in the case of poly(dG)·poly(dC), as is evidenced by alterations of their K_G values. Poly(dA-dT)·poly(dA-dT) in 6 M CsF and poly(dA-dC)·poly(dG-dT) in 4.3 M CsF maintain their inherent conformations in 0.15 M NaCl in spite of the fact that they are characterised by the “X-type” CD-spectrum at these conditions. According to the exchange data the conformation of poly(dA)·poly(dT) in 6 M CsF corresponds to the “heteronomous” DNA model or some other structure with lower accessibility of C8H groups of adenylic residues.     

Experimental and theoretical study of the interaction of single-stranded DNA homopolymers and a monomethine cyanine dye: nature of specific binding.

The photophysical properties of an intercalating unsymmetrical monomethine cyanine dye and single-stranded DNA homopolymers show strong association for poly(dA) and poly(dG), but not for poly(dC) and poly(dT), as determined by several spectroscopic techniques and molecular dynamics calculations. While poly(dA) and poly(dG) appear to bind the dye as a monomer (with dramatic increase in fluorescence), poly(dC) and poly(dT) bind only very weakly, and seem to promote dye aggregation. Only in the case of poly(dA) there seems to be a unique, well defined form of intercalation, that molecular dynamics calculations suggest involve the quinoline ring between two bases, in an arrangement that should favor pi-stacking; consistently with this, the decay of the fluorescence shows a single exponential, the absorption spectrum shows a shift in the dye maximum, the fluorescence is strong, and the induced circular dichroism follows a simple pattern.     

Osmium tetroxide reactivity of DNA bases in nucleotide sequencing and probing of DNA structure.

Osmium tetroxide, 2,2'-bipyridine (Os,bipy) has been widely applied as a probe of the DNA structure. To obtain information about reactivity of DNA bases toward this probe synthetic homopolynucleotides poly(dT), poly(dC), poly(dG) and poly(dA) were treated with Os,bipy and the content of modified bases measured by stripping voltammetry and absorption spectrophotometry. After 20 hours' treatment strong modification of poly(dT) and poly(dC) and weak modification of poly(dG) were observed, while no modification was detected in poly(dA). At short incubation times under conditions close to those usually used in probing the DNA structure the extent of poly(dT) modification was more than 10 times higher than that of poly(dC). Thus, in single-stranded DNA Os,bipy reacts with T much greater than C and G. Due to the fast reaction of thymines with Os,bipy (and osmium tetroxide, pyridine) these chemicals can be applied in Maxam-Gilbert nucleotide sequencing as agents specific for thymines in single-stranded DNA.     

The interactions between the fluorescent dye thiazole orange and DNA

The interaction of the fluorescent dye thiazole orange (TO) with nucleic acids is characterized. It is found that TO binds with highest affinity to double-stranded (ds) DNA [log(K) ≈ 5.5 at 100 mM salt], about 5–10 times weaker to single-stranded polypurines, and further 10–1000 times weaker to single-stranded polypyrimidines. TO binds as a monomer to dsDNAs and poly(dA), both as a monomer and as a dimer to poly(dG) and mainly as a dimer to poly(dC) and poly(dT). The fluorescence quantum yield of TO free in solution is about 2 · 10⁻⁴, and it increases to about 0.1 when bound to dsDNA or to poly(dA), and to about 0.4 when bound to poly(dG). Estimated quantum yields of TO bound to poly(dC) and poly(dT) are about 0.06 and 0.01, respectively. The quantum yield of bound TO depends on temperature and decreases about threefold between 5 and 50°C. © 1998 John Wiley & Sons, Inc. Biopoly 46: 39–51, 1998     

Parallel Double Helices of DNA. Conformational Analysis of Regular Helices with the Second Order Symmetry Axis

Abstract

We have performed a conformational analysis of DNA double helices with parallel directed backbone strands connected with the second order symmetry axis being at the same time the helix axis. The calculations were made for homopolymers poly(dA) · poly(dA), poly(dC) · poly(dC), poly(dG) poly(dG), and poly(dT) · poly(dT). All possible variants of hydrogen bonding of base pairs of the same name were studied for each polymer. The maps of backbone chain geometrical existence were constructed. Conformational and helical parameters corresponding to local minima of conformational energy of “parallel” DNA helices, calculated at atom-atom approximation, were determined. The dependence of conformational energy on the base pair and on the hydrogen bond type was analysed. Two major conformational advantageous for “parallel” DNA's do not depend much on the hydrogen-bonded base pair type were indicated. One of them coincided with the conformational region typical for “antiparallel” DNA in particular for the B-form DNA Conformational energy of “parallel” DNA depends on the base pair type and for the most part is similar to the conformational energy of “antiparallel” B-DNA.     

A UV Resonant Raman Spectroscopic Study of the Interaction of Metallic Derivatives of Tetrakis(4-N-methylpyridyl)porphine with Polynucleotides

Abstract

Resonance Raman spectra excited at 257 nm are reported for the complexes of the Nickel, Cobalt and Zinc derivatives of Tetrakis(4-N-methylpyridyl)porphine with poly(dA.dT)₂, poly(dA)poly(dT), poly(dG.dC)₂ and poly(dG).poly(dC). These spectra are interpreted as evidence of multiple outside binding modes with poly(dA).poly(dT), and of evidence for an outside binding mode with Poly(dG.dC)₂. Some results obtained for the zinc derivative with poly(dA).poly(dT) suggest a binding mode peculiar to this derivative.     

Poly(dG)-poly(dC) DNA appears shorter than poly(dA)-poly(dT) and possibly adopts an A-related conformation on a mica surface under ambient conditions

Three types of DNA: approximately 2700 bp polydeoxyguanylic olydeoxycytidylic acid [poly(dG)-poly(dC)], approximately 2700 bp polydeoxyadenylic polydeoxythymidylic acid [poly(dA)-poly(dT)] and 2686 bp linear plasmid pUC19 were deposited on a mica surface and imaged by atomic force microscopy. Contour length measurements show that the average length of poly(dG)-poly(dC) is approximately 30% shorter than that of poly(dA)-poly(dT) and the plasmid. This led us to suggest that individual poly(dG)-poly(dC) molecules are immobilized on mica under ambient conditions in a form which is likely related to the A-form of DNA in contrast to poly(dA)-poly(dT) and random sequence DNA which are immobilized in a form that is related to the DNA B-form.     

NMR studies of the exocyclic 1,N6-ethenodeoxyadenosine adduct (epsilon dA) opposite thymidine in a DNA duplex. Nonplanar alignment of epsilon dA(anti) and dT(anti) at the lesion site

Two-dimensional proton NMR studies are reported on the complementary d(C-A-T-G-T-G-T-A-C).d(G-T-A-C-epsilon A-C-A-T-G) nonanucleotide duplex (designated epsilon dA.dT 9-mer duplex) containing 1,N6-ethenodeoxyadenosine (epsilon dA), a carcinogen-DNA adduct, positioned opposite thymidine in the center of the helix. Our NMR studies have focused on the conformation of the epsilon dA.dT 9-mer duplex at neutral pH with emphasis on defining the alignment at the dT5.epsilon dA14 lesion site. The through-space NOE distance connectivities establish that both dT5 and epsilon dA14 adopt anti glycosidic torsion angles, are directed into the interior of the helix, and stack with flanking Watson-Crick dG4.dC15 and dG6.dC13 pairs. Furthermore, the d(G4-T5-G6).d(C13-epsilon A14-C15) trinucleotide segment centered about the dT5.epsilon dA14 lesion site adopts a right-handed helical conformation in solution. Energy minimization computations were undertaken starting from six different alignments of dT5(anti) and epsilon dA14(anti) at the lesion site and were guided by distance constraints defined by lower and upper bounds estimated from NOESY data sets on the epsilon dA.dT 9-mer duplex. Two families of energy-minimized structures were identified with the dT5 displaced toward either the flanking dG4.dC15 or the dG6.dC13 base pair. These structures can be differentiated on the basis of the observed NOEs from the imino proton of dT5 to the imino proton of dG4 but not dG6 and to the amino protons of dC15 but not dC13 that were not included in the constraints data set used in energy minimization. Our NMR data are consistent with a nonplanar alignment of epsilon dA14(anti) and dT5(anti) with dT5 displaced toward the flanking dG4.dC15 base pair within the d(G4-T5-G6).d(C13-epsilon A14-C15) segment of the epsilon dA.dT 9-mer duplex.     

Factor D is a selective single-stranded oligodeoxythymidine binding protein.

Factor D, a protein purified from rabbit liver that selectively enhances traversal of template oligodeoxythymidine tracts by diverse DNA polymerases, was examined for the sequence specificity of its binding to DNA. Terminally [32P]-labeled oligomers with the sequence 5'-d[AATTC(N)16G]-3', N being dT, dA, dG, or dC, were interacted with purified factor D and examined for the formation of protein-DNA complexes that exhibit retarded electrophoretic mobility under nondenaturing conditions. Whereas significant binding of factor D to 5'-d[AATTC(T)16G]-3' is detected, there is no discernable association between this protein and oligomers that contain 16 contiguous moieties of dG, dA, or dC. Furthermore, factor D does not form detectable complexes with the duplexes oligo(dA).oligo(dT) or poly(dA).poly(dT). The preferential interaction of factor D with single-stranded poly(dT) is confirmed by experiments in which the polymerase-enhancing activity of this protein is protected by poly(dT) against heat inactivation two- and four-fold more efficiently than by poly(dA) or poly(dA).poly(dT), respectively.     

Minor groove binding of Co(III)meso-tetrakis(N-methylpyridinium-4-yl)porphyrin to various duplex and triplex polynucleotides

The binding site and the geometry of Co(III)meso-tetrakis(N-methylpyridinium-4-yl)porphyrin (CoTMPyP) complexed with double helical poly(dA).poly(dT) and poly(dG).poly(dC), and with triple helical poly(dA).[poly(dT)](2) and poly(dC).poly(dG).poly(dC)(+) were investigated by circular and linear dichroism (CD and LD). The appearance of monomeric positive CD at a low [porphyrin]/[DNA] ratio and bisignate CD at a high ratio of the CoTMPyP-poly(dA).poly(dT) complex is almost identical with its triplex counterpart. Similarity in the CD spectra was also observed for the CoTMPyP-poly(dG).poly(dC) and -poly(dC).poly(dG).poly(dC)(+) complex. This observation indicates that both monomeric binding and stacking of CoTMPyP to these polynucleotides occur at the minor groove. However, different binding geometry of CoTMPyP, when bind to AT- and GC-rich polynucleotide, was observed by LD spectrum. The difference in the binding geometry may be attributed to the difference in the interaction between polynucleotides and CoTMPyP: in the GC polynucleotide case, amine group protrude into the minor groove while it is not present in the AT polynucleotide.     

The incorporation of wrong bases by DNA polymerase I following gamma-irradiation of DNA-like templates

The synthesis of polydeoxyribose polymers by Escherichia coli DNA polymerase I has been investigated with control and gamma-irradiated DNA-like polymer templates containing only two bases. The results show that irradiation of a poly(dA) strand leads to the incorporation of dG, whereas irradiation of poly(dC) and poly(dG) strands both lead to the incorporation of dA. Irradiation of poly(dT) does not lead to the incorporation of any wrong base. The wrong bases are incorporated into the complementary strand of the newly synthesised DNA.     

Variation of DNA sequence specificity of DNA-oligopeptide binding ligands related to netropsin: imidazole-containing lexitropsins

CD binding studies of nonintercalative oligopeptides related to netropsin, named lexitropsins, have been carried out with synthetic duplex DNAs and natural DNA. While netropsin possesses a high dA.dT sequence specificity, these ligands show a progressive lowering of the ability to bind to dA.dT basepairs in DNA and a dramatic reduction of the sequence specificity seen at high salt concentration due to a replacement of pyrrole moieties by imidazoles. This variation in DNA sequence specificity of lexitropsins is mirrored in corresponding large differences in the template inactivation of poly(dA-dT).poly(dA-dT) in the RNA polymerase reaction by these drugs. The presence of imidazole permits binding of the oligopeptide to dG.dC pairs, which is most effective for the triimidazole peptide. Results at increasing salt concentration reveal, however, that a tight binding to pure dG.dC sequences does not occur. A proper sequence containing dG.dC and dA.dT pairs is supposed to be required for a higher specificity. The CD data accord well with previously reported melting studies and are in favor of recent theoretical results suggesting that the diminished AT preference may be due to an increase in the complexation energy with the dG.dC pairs.     

The molecular electrostatic potential of the B-DNA helix. VI. The regions of the base pairs in poly (dG.dC) and poly (dA.dT).

The evaluation of the electrostatic molecular potential at important nucleophilic sites of the purine and pyrimidine bases in poly (dG.dC) and poly (dA.dT) and of the evolution of the potential through the series free bases-nucleosides-nucleotides-single polynucleotide helices-double helices enables the interpretation of the evolution of the corresponding reactivity of the bases towards a series of electrophilic carcinogenic and mutagenic reactants.     

Sedimentation analysis of novel DNA structures formed by homo-oligonucleotides.

Sedimentation velocity analysis has been used to examine the base-specific structural conformations and unusual hydrogen bonding patterns of model oligonucleotides. Homo-oligonucleotides composed of 8-28 residues of dA, dT, or dC nucleotides in 100 mM sodium phosphate, pH 7.4, at 20 degrees C behave as extended monomers. Comparison of experimentally determined sedimentation coefficients with theoretical values calculated for assumed helical structures show that dT and dC oligonucleotides are more compact than dA oligonucleotides. For dA oligonucleotides, the average width (1.7 nm), assuming a cylindrical model, is smaller than for control duplex DNA whereas the average rise per base (0.34 nm) is similar to that of B-DNA. For dC and dT oligonucleotides, there is an increase in the average widths (1.8 nm and 2.1 nm, respectively) whereas the average rise per base is smaller (0.28 nm and 0.23 nm, respectively). A significant shape change is observed for oligo dC(28) at lower temperatures (10 degrees C), corresponding to a fourfold decrease in axial ratio. Optical density, circular dichroism, and differential scanning calorimetry data confirm this shape change, attributable from nuclear magnetic resonance analysis to i-motif formation. Sedimentation equilibrium studies of oligo dG(8) and dG(16) reveal extensive self-association and the formation of G-quadruplexes. Continuous distribution analysis of sedimentation velocity data for oligo dG(16) identifies the presence of discrete dimers, tetramers, and dodecamers. These studies distinguish the conformational and colligative properties of the individual bases in DNA and their inherent capacity to promote specific folding pathways.     

Binding of CC-1065 to poly- and oligonucleotides

The binding of the antitumor agent CC-1065 to a variety of poly- and oligonucleotides was studied by electronic absorption, CD, and resistance to removal by Sephadex column chromatography. Competitive binding experiments between CC-1065 and netropsin were carried out with calf-thymus DNA, poly(dI-dC) · poly(dI-dC), poly(dI) · poly(dC), poly(rA) · poly(dT), poly(dA- dC) · poly(dG-dT), and poly(dA) · 2poly(dT). CC-1065 binds to polynucleotides by three mechanisms. In the first, CC-1065 binds only weakly, as judged by the induction of zero or very weak CD spectra and low resistance to extraction of drug from the polynucleotide by Sephadex chromatography. In the second and third mechanisms, CC-1065 binds strongly, as judged by the induction of two distinct, intense CD spectra and high resistance to extraction of drug from the polynucleotide, by Sephadex chromatography in both cases. The species bound by the second mechanism converts to that bound by the third mechanism with varying kinetics, which depend both on the base-pair sequence and composition of the polynucleotide. Competitive binding experiments with netropsin show that CC-1065 binds strongly in the minor groove of DNA by the second and third mechanisms of binding. Netropsin can displace CC-1065 that is bound by the second mechanism but not that bound by the third mechanism. CC-1065 binds preferentially to B-form duplex DNA and weakly (by the first binding mechanism) or not at all to RNA, DNA, and RNA–DNA polynucleotides which adopt the A-form conformation or to single-strand DNA. This correlation of strong binding of CC-1065 to B-form duplex DNA is consistent with x-ray data, which suggest an anomalous structure for poly(dI) · poly(rC), as compared with poly(rI) · poly(dC) (A-form) and poly(dI) · poly(dC) (B-form). The binding data indicate that poly(rA) · poly(dU) takes the B-form secondary structure like poly(rA) · poly(dT). Triple-stranded poly(dA) · 2poly(dT) and poly(dA) · 2poly(dU), which are considered to adopt the A-form conformation, bind CC-1065 strongly. Netropsin, which also shows a binding preference for B-form polynucleotides, also binds to poly(dA) · 2poly(dT) and occupies the same binding site as CC-1065. These binding studies are consistent with results of x-ray studies, which suggest that A-form triplex DNA retains some structural features of B-form DNA that are not present in A-form duplex DNA; i.e., the axial rise per nucleotide and the base tilt. Triple-stranded poly(dA) · 2poly(rU) does not bind CC-1065 strongly but has nearly the same conformation as poly(dA) · 2poly(dT) based on x-ray analysis. This suggests that the 2′-OH group of the poly(rU) strands interferes with CC-1065 binding to this polynucleotide. The same type of interference may occur for other RNA and DNA–RNA polynucleotides that bind CC-1065 weakly.     

Minor groove binding of Co(III)meso-tetrakis(N-methylpyridinium-4-yl)porphyrin to various duplex and triplex polynucleotides

The binding site and the geometry of Co(III)meso-tetrakis(N-methylpyridinium-4-yl)porphyrin (CoTMPyP) complexed with double helical poly(dA)·poly(dT) and poly(dG)·poly(dC), and with triple helical poly(dA)·[poly(dT)]₂ and poly(dC)·poly(dG)·poly(dC)⁺ were investigated by circular and linear dichroism (CD and LD). The appearance of monomeric positive CD at a low [porphyrin]/[DNA] ratio and bisignate CD at a high ratio of the CoTMPyP-poly(dA)·poly(dT) complex is almost identical with its triplex counterpart. Similarity in the CD spectra was also observed for the CoTMPyP-poly(dG)·poly(dC) and -poly(dC)·poly(dG)·poly(dC)⁺ complex. This observation indicates that both monomeric binding and stacking of CoTMPyP to these polynucleotides occur at the minor groove. However, different binding geometry of CoTMPyP, when bind to AT- and GC-rich polynucleotide, was observed by LD spectrum. The difference in the binding geometry may be attributed to the difference in the interaction between polynucleotides and CoTMPyP: in the GC polynucleotide case, amine group protrude into the minor groove while it is not present in the AT polynucleotide.     

Calculations of stability of A and B forms of dA6.dT6 and dG6.dC6 duplexes by molecular mechanics method in an aqueous solution and approximation of the statistical model. Analysis of unusual stability of the dA6.dT6 B form

The statistical model of the environment for estimating the influence of the aqueous electrolyte solution on the macromolecule has been developed. The energy of the water-fasteners between macromolecule atoms has been calculated. The calculations of A and B form dA6.dT6 and dG6.dC6 duplexes have been made. The unusual stability of B form in dA6.dT6 and their unstability in dG6.dC6 have been analysed. B form duplexes have optimal energy of Van-der-Waals interactions, but a more strained ribose-phosphate backbone, the latter being the reason of its high conformational lability. The aqueous solution stabilizes B form duplexes. The main types of sequence-dependent B form stabilizing interactions are: electrostatic interactions between phosphate groups and bases, the effect of the solvent molecular structure and energy of water fasteners between nucleic bases and ribose-phosphate backbone.