Studies On The Cross Strand Hydrogen Bonds In DNA Double Helices

Abstract

A systematic analysis has been carried out to examine all the stereochemically possible bifurcated hydrogen bonds including those of cross strand type between propeller twisted base pairs in DNA double helices by stereochemical considerations involving base pairs alone and by molecular mechanics studies on dimer and trimer duplexes. The results show that there are limited number of combinations of adjacent base pairs that would facilitate bifurcated cross- strand hydrogen bond (CSH). B-type helices concomitant with negative propeller twist seem to be more favored for the occurrence of CSH than canonical A-type helices because of slide in the latter. The results also demonstrate that helices with appropriate sequences may possess continuous run of these propeller twist driven cross strand hydrogen bonds indicating that they may infact be considered as yet another general structural feature of DNA helices.     

The propeller DNA conformation of poly(dA).poly(dT).

Physical properties of the DNA duplex, poly(dA).poly(dT) differ considerably from the alternating copolymer poly(dAT). A number of molecular models have been used to describe these structures obtained from fiber X-ray diffraction data. The recent solutions of single crystal DNA dodecamer structures with segments of oligo-A.oligo-T have revealed the presence of a high propeller twist in the AT regions which is stabilized by the formation of bifurcated (three-center) hydrogen bonds on the floor of the major groove, involving the N6 amino group of adenine hydrogen bonding to two O4 atoms of adjacent thymine residues on the opposite strand. Here we show that it is possible to incorporate the features of the single crystal analysis, specifically high propeller twist, bifurcated hydrogen bonds, and a narrow minor groove, as well as the close interstrand NMR signal between adenine HC2 and ribose HC1' of the opposite strand, into a model that is fully compatible with the diffraction data obtained from poly(dA).poly(dT).     

Crystal structure of a B-DNA dodecamer containing inosine, d(CGCIAATTCGCG), at 2.4 A resolution and its comparison with other B-DNA dodecamers.

The crystal structure of the dodecamer, d(CGCIAATTCGCG), has been determined at 2.4 A resolution by molecular replacement, and refined to an R-factor of 0.174. The structure is isomorphous with that of the B-DNA dodecamer, d(CGCGAATTCGCG), in space group P2(1)2(1)2(1) with cell dimensions of a = 24.9, b = 40.4, and c = 66.4 A. The initial difference Fourier maps clearly indicated the presence of inosine instead of guanine. The structure was refined with 44 water molecules, and compared to the parent dodecamer. Overall the two structures are very similar, and the I:C forms Watson-Crick base pairs with similar hydrogen bond geometry to the G:C base pairs. The propeller twist angle is low for I4:C21 and relatively high for the I16:C9 base pair (-3.2 degrees compared to -23.0 degrees), and the buckle angles alter, probably due to differences in the contacts with symmetry related molecules in the crystal lattice. The central base pairs of d(CGCIAATTCGCG) show the large propeller twist angles, and the narrow minor groove that characterize A-tract DNA, although I:C base pairs cannot form the major groove bifurcated hydrogen bonds that are possible for A:T base pairs.     

DNA curvature does not require bifurcated hydrogen bonds or pyrimidine methyl groups.

Short tracts of the homopolymer dA.dT confer intrinsic curvature on the axis of the DNA double helix. This phenomenon is assumed to be a consequence of such tracts adopting a stable B'-DNA conformation that is distinct from B-form structure normally assumed by other DNA sequences. The more stable B' structure of dA.dT tracts has been attributed to several possible stabilizing factors: (1) optimal base stacking interactions consequent upon the high propeller twist, (2) bifurcated hydrogen bonds between adjacent dA.dT base-pairs, (3) stacking interactions involving the dT methyl groups, and finally (4) a putative spine of ordered water molecules in the minor groove. DNA oligodeoxynucleotides have been synthesized that enable these hypotheses to be tested; of particular interest is the combination of effects due to bifurcation (2) and methylation of the pyrimidines nucleotides (3). The data indicate that neither bifurcated hydrogen bonds nor pyrimidine methyl groups nor both are essential for DNA curvature. The data further suggest that the influence of the minor groove spine of hydration on the B'-formation is small. The experiments favor the hypothesis that base stacking interactions are the dominant force in stabilizing the B'-form structure.     

Estimation of strength in different extra Watson-Crick hydrogen bonds in DNA double helices through quantum chemical studies

It was shown earlier, from database analysis, model building studies, and molecular dynamics simulations that formation of cross-strand bifurcated or Extra Watson-Crick hydrogen (EWC) bonds between successive base pairs may lead to extra rigidity to DNA double helices of certain sequences. The strengths of these hydrogen bonds are debatable, however, as they do not have standard linear geometry criterion. We have therefore carried out detailed ab initio quantum chemical studies using RHF/6-31G(2d,2p) and B3LYP/6-31G(2p,2d) basis sets to determine strengths of several bent hydrogen bonds with different donor and acceptors. Interaction energy calculations, corrected for the basis set superposition errors, suggest that N-H...O type bent EWC hydrogen bonds are possible along same strands or across the strands between successive base pairs, leading to significant stability (ca. 4-9 kcal/mol). The N-H...N and C-H...O type interactions, however, are not so stabilizing. Hence, consideration of EWC N-H...O H-bonds can lead to a better understanding of DNA sequence directed structural features.     

Structural basis of DNA flexibility

It has been recently shown by us, on the basis of crystal structure database that the flexibility of B-DNA double helices depends significantly on their base sequence. Our model building studies further indicated that the existence of bifurcated cross-strand hydrogen bonds between successive base pairs is possibly the main factor behind the sequence directed DNA flexibility. These cross-strand hydrogen bonds are, of course, weaker than the usual Watson-Crick hydrogen bonds and their bond geometry is characterized by relatively larger bond lengths and smaller bond angles. We have tried to improve our model structures by incorporating non-planarity of the amino groups in DNA bases due to the presence of lone pair electrons at the nitrogen atoms. Energy minimization studies have been carried out by using different quantum chemical methods, whereby it is found that in all cases of N-H....O type cross-strand hydrogen bonds, the bond geometry improves significantly. In the cases of N-H....N type hydrogen bonds, however, no such consistent improvements can be noticed. Perhaps the true picture would emerge only if all the other interactions present in the DNA macromolecule could be appropriately taken into account.     

Solution structure of a dsDNA:LNA triplex

We have determined the NMR structure of an intramolecular dsDNA:LNA triplex, where the LNA strand is composed of alternating LNA and DNA nucleotides. The LNA oligonucleotide binds to the dsDNA duplex in the major groove by formation of Hoogsteen hydrogen bonds to the purine strand of the duplex. The structure of the dsDNA duplex is changed to accommodate the LNA strand, and it adopts a geometry intermediate between A- and B-type. There is a substantial propeller twist between base-paired nucleobases. This propeller twist and a concomitant large propeller twist between the purine and LNA strands allows the pyrimidines of the LNA strand to interact with the 5′-flanking duplex pyrimidines. Altogether, the triplex has a regular global geometry as shown by a straight helix axis. This shows that even though the third strand is composed of alternating DNA and LNA monomers with different sugar puckers, it forms a seamless triplex. The thermostability of the triplex is increased by 19°C relative to the unmodified DNA triplex at acidic pH. Using NMR spectroscopy, we show that the dsDNA:LNA triplex is stable at pH 8, and that the triplex structure is identical to the structure determined at pH 5.1.     

Conformational Effects of DNA Stretching

DNA is an extensible molecule, and an extended conformation of DNA is involved in some biological processes. We have examined the effect of elongation stress on the conformational properties of DNA base pairs by conformational analysis. The calculations show that stretching does significantly affect the conformational properties and flexibilities of base pairs. In particular, we have found that the propeller twist in base pairs reverses its sign upon stretching. The energy profile analysis indicates that electrostatic interactions make a major contribution to the stabilization of the positive-propeller-twist configuration in stretched DNA. This stretching also results in a monotonic decrease in the helical twist angle, tending to unwind the double helix. Fluctuations in most variables initially increase upon stretching, because of unstacking of base pairs, but then the fluctuations decrease as DNA is stretched further, owing to the formation of specific interactions between base pairs induced by the positive propeller twist. Thus, the stretching of DNA has particularly significant effects upon DNA flexibility. These changes in both the conformation and flexibility of base pairs probably have a role in functional interactions with proteins.     

Conformational effects of DNA stretching

DNA is an extensible molecule, and an extended conformation of DNA is involved in some biological processes. We have examined the effect of elongation stress on the conformational properties of DNA base pairs by conformational analysis. The calculations show that stretching does significantly affect the conformational properties and flexibilities of base pairs. In particular, we have found that the propeller twist in base pairs reverses its sign upon stretching. The energy profile analysis indicates that electrostatic interactions make a major contribution to the stabilization of the positive-propeller-twist configuration in stretched DNA. This stretching also results in a monotonic decrease in the helical twist angle, tending to unwind the double helix. Fluctuations in most variables initially increase upon stretching, because of unstacking of base pairs, but then the fluctuations decrease as DNA is stretched further, owing to the formation of specific interactions between base pairs induced by the positive propeller twist. Thus, the stretching of DNA has particularly significant effects upon DNA flexibility. These changes in both the conformation and flexibility of base pairs probably have a role in functional interactions with proteins.     

Probing the role of hydrogen bonds in the stability of base pairs in double-helical DNA

Aromatic stacking and hydrogen bonding between nucleobases are two of the key interactions responsible for stabilization of DNA double-helical structures. The present work aims at defining the specific contributions of these interactions to the stability of individual base pairs in DNA. The two DNA double helices investigated are formed, respectively, by the palindromic base sequences 5'-dCCAACGTTGG-3' and 5'-dCGCAGATCTGCG-3'. The strength of the N==H...N inter-base hydrogen bond in each base pair is characterized from the measurement of the protium-deuterium fractionation factor of the corresponding imino proton using NMR spectroscopy. The structural stability of each base pair is evaluated from the exchange rate of the imino proton, measured by NMR. The results reveal that the fractionation factors of the imino protons in the two DNA double helices investigated fall within a narrow range of values, between 0.92 and 1.0. In contrast, the free energies of structural stabilization for individual base pairs span 3.5 kcal/mol, from 5.2 to 8.7 kcal/mol (at 15 degrees C). These findings indicate that, in the two DNA double helices investigated, the strength of N==H...N inter-base hydrogen bonds does not change significantly depending on the nature or the sequence context of the base pair. Hence, the variations in structural stability detected by proton exchange do not involve changes in the strength of inter-base hydrogen bonds. Instead, the results suggest that the energetic identity of a base pair is determined by the number of inter-base hydrogen bonds, and by the stacking interactions with neighboring base pairs.     

Quantitative structure of a complex between a minor-groove-specific drug and a bent DNA decamer duplex: use of 2D NMR data and NOESY constrained energy minimization

Two-dimensional nuclear magnetic resonance (2D NMR) studies on d(GA4T4C)2 and d(GT4A4C)2 [Sarma, M.H., et al. (1988) Biochemistry 27, 3423-3432; Gupta G., et al. (1988) Biochemistry 27, 7909-7919] showed that A.T pairs are propeller twisted. As a result, A/T tracts form a straight rigid structural block with an array of bifurcated inter base pair H bonds in the major groove. It was demonstrated (previous paper) that replacement of methyl group by hydrogen (changing from T to U) in the major groove does not disrupt the array of bifurcated H bonds in the major groove. In this article, we summarize results of 2D NMR and molecular mechanic studies on the effect of a minor-groove-binding A.T-specific drug on the structure d(GA4T4C)2. A distamycin analogue (Dst2) was used for this study. It is shown that Dst2 binds to the minor groove of d(GA4T4C)2 mainly driven by van der Waals interaction between A.T pairs and the drug; as a consequence, an array of bifurcated H bonds can be formed in the minor groove between amide/amino protons of Dst2 and A.T pairs of DNA. NOESY data suggest that Dst2 predominantly binds at the central 5 A.T pairs. NOESY data also reveal that, upon drug binding, d(GA4T4C)2 does not undergo any significant change in conformation from the free state; i.e., propeller-twisted A.T pairs are still present in DNA and hence the array of bifurcated H bonds must be preserved in the major groove. NOESY data for the A5-T6 sequence also indicate that there is little change in junction stereochemistry upon drug binding.     

Base sequence and helix structure variation in B and A DNA

The observed propeller twist in base-pairs of crystalline double-helical DNA oligomers improves the stacking overlap along each individual helix strand. But, as proposed by Calladine, it also leads to clash or steric hindrance between purines at adjacent base-pairs on opposite strands of the helix. This clash can be relieved by: (1) decreasing the local helix twist angle between base-pairs; (2) opening up the roll angle between base-pairs on the side on which the clash occurs; (3) separating purines by sliding base-pairs along their long axes so that the purines are partially pulled out of the stack (leading to equal but opposite alterations in main-chain torsion angle delta at the two ends of the base-pair); and (4) flattening the propeller twist of the offending base-pairs. Simple sum functions, sigma 1 through sigma 4, are defined, by which the expected local variation in helix twist, base roll angle, torsion angle delta and propeller twist may be calculated from base sequence. All four functions are quite successful in predicting the behavior of B DNA. Only the helix twist and base roll functions are applicable to A DNA, and the helix twist function begins to fail for an A helical RNA/DNA hybrid. Within these limits, the sequence-derived sum functions match the observed helix parameter variation quite closely, with correlation coefficients greater than 0.900 in nearly all cases. Implications of this sequence-derived helix parameter variation for repressor-operator interactions are considered.     

Flexibility of DNA in 2:1 drug-DNA complexes--simultaneous binding of two DAPI molecules to DNA.

Simultaneous binding of two DAPI molecules in the minor groove of (dA)15.(dT)15 B-DNA helix has been simulated by molecular mechanics calculations. The energy minimised structure shows some novel features in relation to binding of DAPI molecules as well as the flexibility of the grooves of DNA helices. The minor groove of the helix expands locally considerably (to 15 angstroms) to accommodate the two DAPI molecules and is achieved by positive propeller twisting of base pairs at the binding site concomitant with small variations in the local nucleotide stereochemistry. The expansion also brings forth simultaneously a contraction in the width of the major groove spread over to a few phosphates. These findings demonstrate another facet of the flexible stereochemistry of DNA helices in which the local features are significantly altered without being propagated beyond a few base pairs, and with the rest of the regions retaining the normal structure. Both the DAPI molecules are engaged in specific hydrogen bonds with the bases and non specific interactions with phosphates. Stacking interactions of DAPI molecules between themselves as well as with sugar-phosphate backbone contribute to the stability of the complex. The studies provide a stereochemical support to the experimental findings that under high drug-DNA ratio DAPI could bind in the 2:1 ratio.     

An NMR structural study of deaminated base pairs in DNA.

The structurally aberrant base pairs TG, UG and TI may occur in DNA as a consequence of deamination of 5-methylcytosine, cytosine and adenine respectively. Results of NMR spectroscopic studies are reported here for these deaminated base pairs in a model seven base pair long oligonucleotide duplex. We find that in all three cases, the DNA helix is a normal B form and both mispaired bases are intrahelical and hydrogen bonded with one another in a wobble geometry. Similarly, in all three cases, all sugars are found to be normal C2' endo in conformation. Symmetric structural perturbations are observed in the helix twist on the 3' side of the mispaired pyrimidine and on the 5' side of the mispaired purine. In all three cases, the amino group of the G residue on the 3' side of the mispaired pyrimidine shows hindered rotation. Although less thermodynamically stable than helices containing only Watson-Crick base pairs, these helices melt normally from the ends and not from the mispair outwards.     

Molecular structure of the netropsin-d(CGCGATATCGCG) complex: DNA conformation in an alternating AT segment

The molecular structure of the complex between a minor groove binding drug (netropsin) and the DNA dodecamer d(CGCGATATCGCG) has been solved and refined by single-crystal X-ray diffraction analysis to a final R factor of 20.0% to 2.4-A resolution. The crystal is similar to that of the other related dodecamers with unit cell dimensions of a = 25.48 A, b = 41.26 A, and c = 66.88 A in the space group P2(1)2(1)2(1). In the complex, netropsin binds to the central ATAT tetranucleotide segment in the narrow minor groove of the dodecamer B-DNA double helix as expected. However, in the structural refinement the drug is found to fit the electron density in two orientations equally well, suggesting the disordered model. This agrees with the results from solution studies (chemical footprinting and NMR) of the interactions between minor groove binding drugs (e.g., netropsin and distamycin A) and DNA. The stabilizing forces between drug and DNA are provided by a combination of ionic, van der Waals, and hydrogen-bonding interactions. No bifurcated hydrogen bond is found between netropsin and DNA in this complex due to the unique dispositions of the hydrogen-bond acceptors (N3 of adenine and O2 of thymine) on the floor of the DNA minor groove. Two of the four AT base pairs in the ATAT stretch have low propeller twist angles, even though the DNA has a narrow minor groove. Alternating helical twist angles are observed in the ATAT stretch with lower twist in the ApT steps than in the TpA step.     

Sequence effects on the propeller twist of base pairs in DNA helices.

Molecular mechanics calculations are performed on all the ten base pair steps (duplex dimers) and also a number of trimer and tetramer duplexes comprising them, in an attempt to systematically examine the possible base sequence effects on the magnitudes of propeller twists of base pairs at a given step. The analysis reveals that though propeller twist is a base pair property, it behaves very much like other base step parameters such as slide, roll, twist etc., Hence, it may be necessary to monitor the nature and variation of magnitudes of pt at a step. Calculations performed on 45 out of the 136 unique tetramer combinations involving all the ten unique base steps show that the difference in magnitudes of propeller twists of the base pairs of a given step has been found to be either steep or moderate depending on base pairs that flank the base step. These observations compare very well with the available experimental data. Tetramer sequences, wherein a base pair of a base step repeats in the same direction, exhibit a relatively steep difference in propeller twist at the step. Tetramers other than these exhibit moderate difference in propeller twist. Such sequences are broadly classified as type-I and type-II respectively. Practically all the tetrads considered in the study, excepting those with GT step and a few involving CG and GC steps, conform to the above classification.     

Sequence Effects On The Propeller Twist Of Base Pairs In DNA Helices

Abstract

Molecular mechanics calculations are performed on all the ten base pair steps (duplex dimers) and also a number of trimer and tetramer duplexes comprising them, in an attempt to systematically examine the possible base sequence effects on the magnitudes of propeller twists of base pairs at a given step. The analysis reveals that though propeller twist is a base pair property, it behaves very much like other base step parameters such as slide, roll, twist etc., Hence, it may be necessary to monitor the nature and variation of magnitudes of pt at a step. Calculations performed on 45 out of the 136 unique tetramer combinations involving all the ten unique base steps show that the difference in magnitudes of propeller twists of the base pairs of a given step has been found to be either steep or moderate depending on base pairs that flank the base step. These observations compare very well with the available experimental data. Tetramer sequences, wherein abase pair of a base step repeats in the same direction, exhibit a relatively steep difference in propeller twist at the step. Tetramers other than these exhibit moderate difference in propeller twist Such sequences are broadly classified as type-I and type-II respectively. Practically all the tetrads considered in the study, excepting those with GT step and a few involving CG and GC steps, conform to the above classification.     

A stable antiparallel cytosine-thymine base pair occurring only at the end of a duplex.

Ultraviolet hyperchromicity experiments indicate that in DNA duplex formation, a C-T mismatch is destabilizing in the center of a duplex, but behaves as a stable base pair at the terminus of a duplex. The C-T base pair is thought to contain two hydrogen bonds, but has thermodynamic parameters (delta Ho and delta Go of dissociation) that are similar to a G-C base pair. AMBER molecular mechanics calculations were performed to study the possible structural properties of DNA duplexes with central and terminal C-T combinations. These calculations also indicate that a central C-T pair destabilizes a duplex, while terminal C-T forms a stable base pair. Hydrogen bonding between cytosine and thymine occurs only in the energy-minimized structures when the helix diameter decreases and the propeller twist angle between the bases increases. These changes are found to occur only at the end of a duplex in the calculations, which may explain the experimental results.     

DNA minor groove recognition of a non-self-complementary AT-rich sequence by a tris-benzimidazole ligand.

The crystal structure of the non-self-complementary dodecamer DNA duplex formed by d(CG[5BrC]ATAT-TTGCG) and d(CGCAAATATGCG) has been solved to 2.3 A resolution, together with that of its complex with the tris-benzimidazole minor groove binding ligand TRIBIZ. The inclusion of a bromine atom on one strand in each structure enabled the possibility of disorder to be discounted. The native structure has an exceptional narrow minor groove, of 2.5-2.6 A in the central part of the A/T region, which is increased in width by approximately 0.8 A on drug binding. The ligand molecule binds in the central part of the sequence. The benzimidazole subunits of the ligand participate in six bifurcated hydrogen bonds with A:T base pair edges, three to each DNA strand. The presence of a pair of C-H...O hydrogen bonds has been deduced from the close proximity of the pyrrolidine group of the ligand to the TpA step in the sequence.     

Stable triple helices are formed upon binding of RNA oligonucleotides and their 2'-O-methyl derivatives to double-helical DNA.

Pyrimidine oligoribonucleotides bind to the major groove of double-helical DNA at homopurine.homopyrimidine sequences. They recognize Watson-Crick base pairs by forming T.A x U and C.G x C base triplets via Hoogsteen hydrogen bonding. The stability of these triple helices is much higher than that of triple helices formed by oligodeoxyribonucleotides as shown by an increase of the temperature at which half-dissociation of the third strand occurs. When the 2'-hydroxyl group of ribose moieties is replaced by 2'-O-methyl substituent, triple helix stability is further increased.