Structure of DNA sequence d-TGATCA by two-dimensional nuclear magnetic resonance spectroscopy and restrained molecular dynamics

The 5' d-TpG 3' element is a part of DNA sequences involved in regulation of gene expression and is also a site for intercalation of several anticancer drugs. Solution conformation of DNA duplex d-TGATCA containing this element has been investigated by two-dimensional NMR spectroscopy. Using a total of 12 torsional angles and 121 distance constraints, structural refinement has been carried out by restrained molecular dynamics (rMDs) in vacuum up to 100 ps. The structure is characterized by a large positive roll at TpG/CpA base pair step and large negative propeller twist for AT and TA base pairs. The backbone torsional angle, gamma(O5'-C5'-C4'-C3'), of T1 residue adopts a trans-conformation which is corroborated by short intra nucleotide T1H6-T1H5' (3.7A) distance in nuclear overhauser effect spectroscopy (NOESY) spectra while the backbone torsional angle, beta(P-O5'-C5'-C4'), exists in trans as well as gauche state for T1 and C5 residues. There is evidence of significant flexibility of the sugar-phosphate backbone with rapid inter-conversion between two different conformers at TpG/CpA base pair step. The base sequence dependent variations and local structural heterogeneity have important implications in specific recognition of DNA by ligands.     

Sequence dependence of DNA conformational flexibility

By using conformational free energy calculations, we have studied the sequence dependence of flexibility and its anisotropy along various conformational variables of DNA base pairs. The results show the AT base step to be very flexible along the twist coordinate. On the other hand, homonucleotide steps, GG(CC) and AA(TT), are among the most rigid sequences. For the roll motion that would correspond to a bend, the TA step is most flexible, while the GG(CC) step is least flexible. The flexibility of roll is quite anisotropic; the ratio of fluctuations toward the major and minor grooves is the largest for the GC step and the smallest for the AA(TT) and CG steps. Propeller twisting of base pairs is quite flexible, especially of A.T base pairs; propeller twist can reach 19 degrees by thermal fluctuation. We discuss the effect of electrostatic parameters, comparison with available experimental results, and biological relevance of these results.     

A two-base-pair substitution in T7 promoter by SP6 promoter-specific base pairs alone abolishes T7 promoter activity but reveals SP6 promoter activity.

The phage T7 and SP6 RNA polymerase-promoter systems are very similar in many characteristics, but maintains stringent specificity for each. In order to identify the base pair element that distinguishes between T7 and SP6 promoters, the base pairs at -12, -10, -9, and -8 of the T7 promoter consensus sequence were changed singly and multiply to the SP6 promoter-specific base pairs, and assayed for T7 and SP6 promoter activities. The results indicate that the primary discrimination element is the base pairs at -8 and -9. The two-base-pair substitution alone in T7 promoter by SP6-specific base pairs is sufficient to make the T7 variant be a SP6 promoter, abolishing T7 promoter activity.     

Oxetane locked thymidine in the Dickerson-Drew dodecamer causes local base pairing distortions -- an NMR structure and hydration study

The introduction of a North-type sugar conformation constrained oxetane T block, 1-(1',3'-O-anhydro-beta-D-psicofuranosyl) thymine, at the T(7) position of the self-complementary Dickerson-Drew dodecamer, d[(5'-C(1)G(2)C(3)G(4)A(5)A(6)T(7)T(8)C(9)G(10)C(11)G(12)-3')](2), considerably perturbs the conformation of the four central base pairs, reducing the stability of the structure. UV spectroscopy and 1D NMR display a drop in melting temperature of approximately 10 degrees C per modification for the T(7) oxetane modified duplex, where the T(7) block has been introduced in both strands, compared to the native Dickerson-Drew dodecamer. The three dimensional structure has been determined by NMR spectroscopy and has subsequently been compared with the results of 2.4 ns MD simulations of the native and the T(7) oxetane modified duplexes. The modified T(7) residue is found to maintain its constrained sugar- and the related glycosyl torsion conformations in the duplex, resulting in staggered and stretched T(7).A(6) and A(6).T(7) non-linear base pairs. The stacking is less perturbed, but there is an increased roll between the two central residues compared to the native counterpart, which is compensated by tilts of the neighboring base steps. The one dimensional melting profile of base protons of the T(7) and T(8) residues reveals that the introduction of the North-type sugar constrained thymine destabilizes the core of the modified duplex, promoting melting to start simultaneously from the center as well as from the ends. Temperature dependent hydration studies by NMR demonstrate that the central T(7).A(6)/A(6).T(7) base pairs of the T(7) oxetane modified Dickerson-Drew dodecamer have at least one order of magnitude higher water exchange rates (correlated to the opening rate of the base pair) than the corresponding base pairs in the native duplex.     

Base interaction and conformation manifestations of repetitive nucleotide sequences

To understand why different nucleotide sequences prefer different double helical conformations and to predict conformational behaviour of definite sequences the base-base interaction energy in regular helices consisting of A:U, A:T, G:C and I:C (hypoxanthine-cytosine) base pairs was calculated. Interaction energy was assumed to be a function of eight conformational parameters: H, the distance between adjacent pairs along helix axes; tau, turn angle of one pair relative to the neighbouring one; angles between base planes in a pair (TW, propeller twist and BL, buckle) and position of pairs with respect to helix axes (D and SL, displacements in the plane normal to helix axes, and TL and RL, inclinations to this plane, tilt and roll, respectively). For H and tau characteristic of A- and B-families of nucleic acid conformations (2.5 A less than H less than or equal to 3.5 A, 30 degrees less than or equal to tau less than or equal to 45 degrees) the ranges of conformational parameters corresponding to energy values close to minimal ones (valleys) and correlations between conformational parameters were revealed. Valleys for different sequences largely coincide but have distinctive characteristics for each sequence. Reasons for base pair planarity distortion in double-stranded helices were considered. The calculations permit to account for A-phility of G:C sequences and B-phility for A:T sequences. The valley for I:C sequence branches. This corresponds to A:T-like behaviour in some cases and G:C-like in the others.     

Helix bending as a factor in protein/DNA recognition

Normal vectors perpendicular to individual base pairs are a powerful tool for studying the bending behavior of B-DNA, both in the form of normal vector plots and in matrices that list angles between vectors for all possible base pair combinations. A new analysis program, FREEHELIX, has been written for this purpose, and applied to 86 examples of sequence-specific protein/DNA complexes whose coordinates are on deposit in the Nucleic Acid Data Base. Bends in this sample of 86 structures almost invariably follow from roll angles between adjacent base pairs; tilt makes no net contribution. Roll in a direction compressing the broad major groove is much more common than that which compresses the minor groove. Three distinct types of B-DNA bending are observed, each with a different molecular origin: (1) Localized kinking is produced by large roll at single steps or at two steps separated by one turn of helix. (2) Smooth, planar curvature is produced by positive and negative roll angles spaced a half-turn apart, with random side-to-side zigzag roll at intermediate points, rather than a tilt contribution that might have been expected theoretically. (3) Three-dimensional writhe results from significant roll angles at a continuous series of steps. Writhe need not change the overall direction of helix axis, if it is continued indefinitely or for an integral number of helical turns. A-DNA itself can be formally considered as possessing uniform, continuous writhe that yields no net helix bending. Smooth curvature is the most intricate deformation of the three, and is least common. Writhe is the simplest deformation and is most common; indeed, a low level of continuous writhe is the normal condition of an otherwise unbent B-DNA helix of general sequence. With one exception, every example of major kinking in this sample of 86 structures involves a pyrimidine–purine step: C–A/T–G, T–A, or C–G. Purine–purine steps, especially A–A, show the least tendency toward roll deformations. © 1998 John Wiley & Sons, Inc. Biopoly 44: 361–403, 1997     

Domain structure of the simian virus 40 core origin of replication.

The simian virus 40 core origin of replication consists of nucleotides 5211 through 31. These 64 base pairs contain three functional domains with strict sequence requirements and two spacer regions with relaxed sequence specificity but precise positional constraints. The early domain extends for 10 contiguous base pairs between nucleotides 5211 and 5220. A 9-base pair spacer from sequences 5221 through 5229 separates the early domain from the 23-base pair central palindrome that directs the binding of T antigen. The late end of the core between nucleotides 12 and 31 also contains spacer and sequence-specific functions that are not yet completely mapped. We propose that the sequence-specific domains are interaction sites for viral and cellular proteins, determinants of DNA conformation, or both. The spacers would position these signals at required distances and rotations relative to one another.     

DNA bending: the prevalence of kinkiness and the virtues of normality.

DNA bending in 86 complexes with sequence-specific proteins has been examined using normal vector plots, matrices of normal vector angles between all base pairs in the helix, and one-digit roll/slide/twist tables. FREEHELIX, a new program especially designed to analyze severely bent and kinked duplexes, generates the foregoing quantities plus local roll, tilt, twist, slide, shift and rise parameters that are completely free of any assumptions about an overall helix axis. In nearly every case, bending results from positive roll at pyrimidine-purine base pair steps: C-A (= T-G), T-A, or less frequently C-G, in a direction that compresses the major groove. Normal vector plots reveal three well-defined types of bending among the 86 examples: (i) localized kinks produced by positive roll at one or two discrete base pairs steps, (ii) three-dimensional writhe resulting from positive roll at a series of adjacent base pairs steps, or (iii) continuous curvature produced by alternations of positive and negative roll every 5 bp, with side-to-side zig-zag roll at intermediate position. In no case is tilt a significant component of the bending process. In sequences with two localized kinks, such as CAP and IHF, the dihedral angle formed by the three helix segments is a linear function of the number of base pair steps between kinks: dihedral angle = 36 degrees x kink separation. Twenty-eight of the 86 examples can be described as major bends, and significant elements in the recognition of a given base sequence by protein. But even the minor bends play a role in fine-tuning protein/DNA interactions. Sequence-dependent helix deformability is an important component of protein/DNA recognition, alongside the more generally recognized patterns of hydrogen bonding. The combination of FREEHELIX, normal vector plots, full vector angle matrices, and one-digit roll/slide/twist tables affords a rapid and convenient method for assessing bending in DNA.     

Massive parallel analysis of DNA-Hoechst 33258 binding specificity with a generic oligodeoxyribonucleotide microchip.

A generic oligodeoxyribonucleotide microchip was used to determine the sequence specificity of Hoechst 33258 binding to double-stranded DNA. The generic microchip contained 4096 oxctadeoxynucleo-tides in which all possible 4(6)= 4096 hexadeoxy-nucleotide sequences are flanked on both the 3'- and 5'-ends with equimolar mixtures of four bases. The microchip was manufactured by chemical immobilization of presynthesized 8mers within polyacrylamide gel pads. A selected set of immobilized 8mers was converted to double-stranded form by hybridization with a mixture of fluorescently labeled complementary 8mers. Massive parallel measurements of melting curves were carried out for the majority of 2080 6mer duplexes, in both the absence and presence of the Hoechst dye. The sequence-specific affinity for Hoechst 33258 was calculated as the increase in melting temperature caused by ligand binding. The dye exhibited specificity for A:T but not G:C base pairs. The affinity is low for two A:T base pairs, increases significantly for three, and reaches a plateau for four A:T base pairs. The relative ligand affinity for all trinucleotide and tetranucleotide sequences (A/T)(3)and (A/T)(4)was estimated. The free energy of dye binding to several duplexes was calculated from the equilibrium melting curves of the duplexes formed on the oligonucleotide microchips. This method can be used as a general approach for massive screening of the sequence specificity of DNA-binding compounds.     

DNA Sequence Analysis of Mutagenicity and Site Specificity of Ethyl Methanesulfonate in Uvr+ and UvrB - Strains of ESCHERICHIA COLI

EMS-induced mutations within a 180 base pair region of the lacI gene of E. coli were cloned and sequenced. In total, 105 and 79 EMS-induced mutations from a Uvr+ and a UvrB- strain, respectively, were sequenced. The specificity of EMS-induced mutagenesis was very similar in the two strains; G:C----A:T transitions accounted for all but three of the mutants. The overall frequency of induced mutation was fivefold higher in the UvrB- strain compared to the Uvr+ strain. This demonstrates, at the DNA sequence level, that the presumed premutagenic lesion, O6-ethylguanine, is subject to repair by the uvrABC excision repair system of E. coli. An analysis of mutation frequencies with respect to neighboring base sequence, in the two strains, shows that O6-ethylguanine lesions adjacent to A:T base pairs present better targets for the excision repair machinery than those not adjacent to A:T base pairs.     

Effect of base-pair sequence on the conformations and thermally induced transitions in oligodeoxyribonucleotides containing only AT base pairs

Tm curves, CD spectra, and kinetics results of the self-complementary DNA dodecamers d(A6T6), d(A3T3A3T3), d(A2T2A2T2A2T2), d(ATATATATATAT), and d(T6A6) demonstrate that the thermal transitions of these oligomers at low salt concentration involve a hairpin intermediate. At high salt concentrations (greater than 0.1 M Na+) only a duplex to denatured-strand transition appears to occur. The temperature and salt-concentration regions of the transitions are very sequence dependent. Alternating-type AT sequences have a lower duplex stability and a greater tendency to form hairpins than sequences containing more nonalternating AT base pairs. Of the two nonalternating sequences, d(T6A6) is significantly less stable than d(A6T6). Both oligomers have CD curves that are very similar to the unusual CD spectrum of poly(dA).poly(dT). The Raman spectra of these two oligomers are also quite similar, but at low temperature, small intensity differences in two backbone modes and three nucleoside vibrations are obtained. The hairpin to duplex transition for the AT dodecamers was examined by salt-jump kinetics measurements. The transition is faster than transitions for palindromic-sequence oligomers containing terminal GC base pairs. Stopped-flow kinetics studies indicate that the transition is second order and has a relatively low activation energy. The reaction rate increases with increasing ionic strength. These results are consistent with a three-step mechanism for the hairpin to duplex reaction: (i) fraying of the hairpin oligomers' terminal base pairs, (ii) a rate-determining bimolecular step involving formation of a cruciform-type intermediate from two hairpin oligomers with open terminal base pairs, and (iii) base-pair migration and formation in the intermediate to give the duplex.     

Isostericity and tautomerism of base pairs in nucleic acids

The natural bases of nucleic acids form a great variety of base pairs with at least two hydrogen bonds between them. They are classified in twelve main families, with the Watson–Crick family being one of them. In a given family, some of the base pairs are isosteric between them, meaning that the positions and the distances between the C1′ carbon atoms are very similar. The isostericity of Watson–Crick pairs between the complementary bases forms the basis of RNA helices and of the resulting RNA secondary structure. Several defined suites of non-Watson–Crick base pairs assemble into RNA modules that form recurrent, rather regular, building blocks of the tertiary architecture of folded RNAs. RNA modules are intrinsic to RNA architecture are therefore disconnected from a biological function specifically attached to a RNA sequence. RNA modules occur in all kingdoms of life and in structured RNAs with diverse functions. Because of chemical and geometrical constraints, isostericity between non-Watson–Crick pairs is restricted and this leads to higher sequence conservation in RNA modules with, consequently, greater difficulties in extracting 3D information from sequence analysis. Nucleic acid helices have to be recognised in several biological processes like replication or translational decoding. In polymerases and the ribosomal decoding site, the recognition occurs on the minor groove sides of the helical fragments. With the use of alternative conformations, protonated or tautomeric forms of the bases, some base pairs with Watson–Crick-like geometries can form and be stabilized. Several of these pairs with Watson–Crick-like geometries extend the concept of isostericity beyond the number of isosteric pairs formed between complementary bases. These observations set therefore limits and constraints to geometric selection in molecular recognition of complementary Watson–Crick pairs for fidelity in replication and translation processes.     

Z-curve: a computer program calculating DNA helical axis coordinates for three-dimensional graphic presentation of curvature.

In order to predict curvature of DNA fragments, we previously developed a computer program for simply calculating a vectorial sum of all individual roll, tilt and twist wedge angles between the nearest base pairs for a given DNA fragment [Lee et al., (1991)]. Now, a new program, called Z-curve, was developed to calculate three-dimensional coordinates of the helical center of each base pair along the DNA, using helical axis deviations from B-form DNA by wedge angles. The output file of the new program was designed to become an input file for a graphics program, Insight II. Thus, we were able to obtain three-dimensional graphic presentations of DNA helical axis curvatures of any length. It visualized spatial details of the DNA curvature, where and how much it curves, and to which direction. It also allowed calculation of the three-dimensional distance between two ends of a DNA fragment, which could provide a measure of its curvature. Here, three DNA fragments, both curved and straight, were subjected to the Z-curve and Insight II programs. The results showed that their curvature details could be visualized to the level of the base pair, whether the DNA fragments contained an oligo(A) track or not. Their estimated curvatures were consistent with the experimental results of permutation gel mobility assay.     

Mismatches in DNA double strands: thermodynamic parameters and their correlation to repair efficiencies.

The helix-coil transitions of the 16 octadecameric DNA duplexes dCGTCGTTTXACAACGTCG X dCGACGTTGTX1AAACGACG with A, T, G, and C for X and X1 were measured by UV-absorption. This sequence was taken from former studies of in vivo determination of efficiencies of mismatch repair (Kramer, Kramer, and Fritz (1984) Cell 38, 879-887). The thermodynamic parameters for double strand and mismatch formation have been obtained by evaluating the partition function of a stack model which allowed for loop formation. As a result the mismatches could be classified into wobble base pairs (T/G, G/G, C/A, A/A, A/G), open base pairs, i.e. permanent loops (T/T, C/T, T/C, C/C), and intermediate or weak base pairs (G/T, A/C, G/A). There is no correlation between Tm and the biological repair efficiency of X/X1. The structure classes, however, as described above show a close correlation: Open base pairs show the lowest repair efficiencies, whereas mismatches with high repair efficiency always belong to the structural class of wobble base pairs. Because of the palindromic nearest neighbors of the variation site X/X1, the influence of next-nearest neighbor interactions could be detected and be estimated to about 1 kJ/mol for one stack.     

NMR structure of a parallel-stranded DNA duplex at atomic resolution

DNA dodecamers have been designed with two cytosines on each end and intervening A and T stretches, such that the oligomers have fully complementary A:T base pairs when aligned in the parallel orientation. Spectroscopic (UV, CD and IR), NMR and molecular dynamics studies have shown that oligomers having the sequences d(CCATAATTTACC) and d(CCTATTAAATCC) form a parallel-stranded duplex when dissolved at 1:1 stoichiometry in aqueous solution. This is due to the C:C⁺ clamps on either end and extensive mismatches in the antiparallel orientation. The structure is stable at neutral and acidic pH. At higher temperatures, the duplex melts into single strands in a highly cooperative fashion. All adenine, cytosine and thymine nucleotides adopt the anti conformation with respect to the glycosidic bond. The A:T base pairs form reverse Watson–Crick base pairs. The duplex shows base stacking and NOEs between the base protons T(H6)/A(H8) and the sugar protons (H1′/H2′/H2″) of the preceding nucleotide, as has been observed in antiparallel duplexes. However, no NOEs are observed between base protons H2/H6/H8 of sequential nucleotides, though such NOEs are observed between T(CH₃) and A(H8). A three-dimensional structure of the parallel-stranded duplex at atomic resolution has been obtained using molecular dynamics simulations under NMR constraints. The simulated structures have torsional angles very similar to those found in B-DNA duplexes, but the base stacking and helicoid parameters are significantly different.     

Modelling basic features of specificity in the binding of a dicationic steroid diamine to double-stranded oligonucleotides.

An investigation of the intrinsically preferred binding modes of a steroid diamine, dipyrandium, to the double-stranded hexanucleotides d(TATATA)2, d(ATATAT)2, and d(CGCGCG)2 is carried out by the energy minimization procedure JUMNA. Several alternative binding modes are compared: groove binding in which the conformation of the oligonucleotide remains close to that of B-DNA, intercalation between base-pairs and interaction with variously kinked structures in which base pairs of dinucleoside steps open towards the groove in which the binding occurs. The favored binding configuration occurs at the d(TpA) step of the AT kinked nucleotides in which the kink opens the base pairs towards the minor groove. Thus, for the d(T1A2T3A4T5A6)2 sequences the preferred complexation involves the kink at the T3A4 step facing the cyclohexane rings A, B, and C of the ligand. For the d(A1T2A3T4A5T6)2 sequence, the kink occurs at the T2A3 step facing the cationic pyrrolidine ring linked to ring A. The binding of dipyrandium to d(CGCGCG)2 is found to be considerably less favourable than for either of the two (AT) sequences.     

A Stochastic Model for Helix Bending in B-DNA

Abstract

Bending in double-helical B-DNA apparently occurs only by rolling adjacent base pairs over one another along their long axes. The lifting apart of ends that would be required by tilt or wedge angle contributions is too costly in free energy and does not occur. Roll angles at base steps can be positive (compression of major groove) or negative (compression of minor groove); with the former somewhat easier.

Individual steps may advance or oppose the overall direction of bend, or make lateral excursions, but the result of this series of “random roll” steps is the production of a net bending in the helix axis. Because the natural roll points for bending in a given plane occur every 5 base pairs, one would expect that double-helical DNA wrapped around a nucleosome core would exhibit bends with the same periodicity. Alternate bends might be particularly acute where the major groove faced the nucleosome core and was compressed against it.

The “annealed kinking” model proposed by Fratini et al. (J. Biol. Chem. 257, 14686 (1982) was suggested from the observation that a major bend at a natural roll point is flanked by decreasing roll angles at the steps to either side, as though local strain was being minimized by somewhat blurring the bend out rather than keeping it localized. The random walk model suggested in this paper would describe this as a decreased roll angle as the helix step rotates toward a direction perpendicular to the overall bend. Bending of DNA is seen to be a more stochastic process than had been suspected. Detailed analysis of every helix step reveals both side excursions and backward or retrograde motion, as in any random walk situation. Yet these isolated steps counteract one another, to leave behind a residuum of overall bending in a specific direction.     

Solution structure of the TnAn DNA duplex GCCGTTAACGCG containing the HpaI restriction site.

The solution structure of the self-complementary DNA duplex [d(GCCGTTAACGGC)]2, which contains the HpaI restriction site GTTAAC, has been elucidated by two-dimensional NMR, distance geometry (DG), and NOE back-calculation methods. Initial distance constraints were determined by polynomial fitting the two-spin initial NOE rates; backbone constraints from NOE and J-coupling observations (Kim et al., 1992) were included. RMSDs between initial-distance-refined structures derived from random-embedded DG, A-DNA, and B-DNA starting structures were all in the range 0.5-1.0 A, indicating good convergence properties of the algorithm, regardless of the starting structure. A semiautomatic back-calculation refinement procedure was developed and used to generate more refined structures for which the BKCALC-simulated NOE volumes matched the experimental data. The six final structures refined from various starting structures exhibit very good agreement with the experimental data (R values = 0.18) and converge well to within 0.8-A RMSD differences for the central 8 base pairs. The torsion and pseudorotation phase angles were found to be well determined by the data, and the local helical parameters for each base step converged quite well. The final structures show that the central T6-A7 step is somewhat underwound (twist angle ca. 29 degrees), with a large negative cup and a normal (wide) minor groove width, while the T5-T6 and A7-A8 steps have a partially narrowed minor groove.     

IS4 is found between eleven or twelve base pair duplications

Summary Three mutations caused by the integration of IS4 in galT in both possible orientations were shown by DNA sequence analysis to be integrated between a duplication of eleven base pairs of gene galT.IS4 has been cloned from its single position on the E. coli K12 chromosome. Here, 12 base pairs are duplicated adjacent to IS4. This sequence is unrelated to the duplicated sequence in galT.