An NMR study of d(CTACTGCTTTAG).d(CTAAAGCAGTAG) showing hydration water molecules in the minor groove of a TpA step

The hydration properties of the non-palindromic duplex d(CTACTGCTTTAG). d(CTAAAGCAGTAG) were investigated by NMR spectroscopy. The oligonucleotide possesses a heterogeneous B-DNA structure. The H2(n)-H1'(m+1) distances reflect a minor groove narrowing within the TTT/AAA segment (approximately 3.9A) and a sudden widening at the T10:A15 base-pair (approximately 5.3A), the standard B-DNA distance being approximately 5A. The facing T10pA11 and T14pA15 steps at the end of the TTTA/AAAT segment have completely different behaviors. Only A15 ending the AAA run displays NMR features comparable to those shown by adenines of TpA steps occupying the central position of TnAn (n> or =2) segments. These involve particular chemical shifts and line broadening of the H2 and H8 protons. Positive NOESY cross-peaks were measured between the water protons and the H2 protons of A15, A16 and A17 reflecting the occurrence of hydration water molecules with residence times longer than 500 picoseconds along the minor groove of the TTT/AAA segment. In contrast no water molecules with long residence times were observed neither for A3, A20 and A23 nor for A11 ending the 5'TTTA run. We confirm thus that the binding of water molecules with long residence time to adenine residues correlates with the minor groove narrowing. In contrast, the widening of the minor groove at the A11:T14 base-pair ending the TTTA/TAAA segment, likely associated to a high negative propeller twist value at this base-pair, prevents the binding of a water molecule with long residence time to A11 but not to A15 of the preceding T10:A15 base-pair. Thus, in our non-palindromic oligonucleotide the water molecules bind differently to A11 and A15 although both adenines are part of a TpA step. The slower motions occurring at A15 compared to A11 are also well explained by the present results.     

Compensating bends in a 16-base-pair DNA oligomer containing a T(3)A(3) segment: A NMR study of global DNA curvature

In-phase ligated DNA containing T(n)A(n) segments fail to exhibit the retarded polyacrylamide gel electrophoresis (PAGE) migration observed for in-phase ligated A(n)T(n) segments, a behavior thought to be correlated with macroscopic DNA curvature. The lack of macroscopic curvature in ligated T(n)A(n) segments is thought to be due to cancellation of bending in regions flanking the TpA steps. To address this issue, solution-state NMR, including residual dipolar coupling (RDC) restraints, was used to determine a high-resolution structure of [d(CGAGGTTTAAACCTCG)2], a DNA oligomer containing a T3A3 tract. The overall magnitude and direction of bending, including the regions flanking the central TpA step, was measured using a radius of curvature, Rc, analysis. The Rc for the overall molecule indicated a small magnitude of global bending (Rc = 138 +/- 23 nm) towards the major groove, whereas the Rc for the two halves (72 +/- 33 nm and 69 +/- 14 nm) indicated greater localized bending into the minor groove. The direction of bending in the regions flanking the TpA step is in partial opposition (109 degrees), contributing to cancellation of bending. The cancellation of bending did not correlate with a pattern of roll values at the TpA step, or at the 5' and 3' junctions, of the T3A3 segment, suggesting a simple junction/roll model is insufficient to predict cancellation of DNA bending in all T(n)A(n) junction sequence contexts. Importantly, Rc analysis of structures refined without RDC restraints lacked the precision and accuracy needed to reliably measure bending.     

Structural comparison of the B-DNA dodecamers d(CGCGTTAACGCG) and d(CGCGAATTCGCG) with T2A2 and A2T2 tracts.

The x-ray structure of the deoxy oligonucleotide dodecamer d(CGCGTTAACGCG) recently determined in our laboratory shows that the helical parameters of the central TTAA segment are significantly different compared to the central AATT in d(CGCGAATTCGCG). The roll in the central TA step of the T2A2 dodecamer opens towards the minor groove while the AT step of the A2T2 dodecamer opens towards the major groove. Also, the roll angles at the steps 4 and 8 (GT and AC in T2A2) and (GA and TC in A2T2) are in opposite directions. The high cup and helical twist angles at the central base-pair of T2A2 decreases the base stacking interactions compared to A2T2. Tilt angles within the tetranucleotide segments TTAA and AATT have opposite signs. In spite of the local differences caused by the sequence inversion (TTAA----AATT), the two dodecamers exhibit similar overall bending. The top third is more bent than the bottom third relative to the central segment. This asymmetric bending in the two dodecamers is mainly due to crystal packing interactions.     

Binding of a Hoechst dye to d(CGCGATATCGCG) and its influence on the conformation of the DNA fragment

Hoechst dye 33258 is a planar drug molecule that binds to the minor groove of DNA, especially where there are a number of A.T base pairs. We have solved the structure of the Hoechst dye bound to the DNA dodecamer d(CGCGATATCGCG) at 2.3 A. This structure is compared to that of the same dodecamer with the minor-groove-binding drug netropsin bound to it, as well as to structures that have been solved for this Hoechst dye bound to a DNA dodecamer containing the central four base pairs with the sequence AATT. We find that the position of the Hoechst drug in this dodecamer is quite different from that found in the other dodecamer since it has an opposite orientation compared to the other two structures. The drug covers three of the four A.T base pairs and extends its piperazine ring to the first G.C base pair adjacent to the alternating AT segment. Furthermore, the drug binding has modified the structure of the DNA dodecamer. Other DNA dodecamers with alternating AT sequences show an alternation in the size of the helical twist between the ApT step (small twist) and the TpA step (large twist). In this structure the alternation is reversed with larger twists in the ApT steps than in the TpA step. In addition, there is a rotation of one of the thymine bases in the DNA dodecamer that is associated with hydrogen bonding to the Hoechst drug. This structure illustrates the considerable plasticity found in the DNA molecule when it binds to different planar molecules inserted into the minor groove.     

NMR evidence for base dynamics at all TpA steps in DNA

NMR evidence is presented indicating that the exceptional conformational dynamics found at TpA steps in DNA is general to all immediate sequence contexts. One easily tractable NMR parameter that is sensitive to TpA base dynamics is the resonance linewidth of the TpA adenine H2 proton. This resonance experiences a temperature-dependent broadening due to conformational dynamics. Unusual dynamics at TpA steps were originally observed in the sequence context (T)pTpTpApAp(A). We have since shown that the evidence for TpA dynamics persists when either the thymine preceding the TpA step or the adenine following the TpA step is preserved [McAteer et al., Nucleic Acids Res. 23, 3962-3966 (1995)]. Here, in order establish whether or not exceptional TpA dynamics occurs in all DNA sequence contexts, we investigated a series of DNA sequences of the form GCNaTANbNbTANaGC, where N=A,T,C,G. In this family of sequences, all 16 possible immediate sequence context environments of the form NaTANb were examined using 10 DNA sequences. Our NMR results show that the TpA adenine H2 resonance contains a temperature dependent excess linewidth indicative of dynamics in all 16 sequence context environments. By studying a complete set of sequence contexts, it was possible to recognize trends relating resonance parameters and sequence environment. For example, the magnitude of the maximum linewidth is largely determined by the identity of the nucleotide following the TpA step and the magnitude of the linewidth maximum is moderately correlated (r=0.56) with the temperature of the linewidth maximum. The physical basis for these correlations is discussed.     

Structural variation in d(CTCTAGAG). Implications for protein-DNA interactions

Single-crystal X-ray diffraction techniques have been used to characterize the structure of the self-complementary DNA oligomer d(CTCTAGAG). The structure was refined to an R factor of 14.7% using data to 2.15-A resolution. The tetragonal unit cell, space group P4(3)2(1)2, has dimensions a = 42.53 and c = 24.33 A. The asymmetric unit consists of a single strand or four base pairs. Two strands, related by a crystallographic dyad axis, coil about each other to form a right-handed duplex. This octamer duplex has a mean helix rotation of 32 degrees, 11.3 base pairs per turn, an average rise of 3.1 A, C3'-endo furanose conformations, a shallow minor groove, and a deep major groove. Such averaged parameters suggest classification of the octamer as a member of the A-DNA family. However, the global parameters tend to mask variations in conformational parameters observed at the level of the base pairs. In particular, the central TpA (= TpA) step displays extensive interstrand purine-purine overlap and an unusual sugar-phosphate backbone conformation. These structural features may be directly related to certain sequence-specific protein-DNA interactions involving nucleases and repressors.     

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.     

The effects of sequence context on base dynamics at TpA steps in DNA studied by NMR.

Base dynamics, heretofore observed only at TpA steps in DNA, were investigated as a function of sequence context by NMR spectroscopy. The large amplitude conformational dynamics have been previously observed in TnAn segments where n > or = 2. In order to determine whether the dynamic characteristics occur in more general sequence contexts, we examined four self-complementary DNA sequences, [d(CTTTA-NATNTAAAG)2] (where N = A, C, T, G and N = complement of N). The anomalous broadening of the TpA adenine H2 resonance which is indicative of large amplitude base motion was observed in all nine unique four nucleotide contexts. Furthermore, all the adenine H2 resonances experienced a linewidth maximum as a function of temperature, which is a characteristic of the dynamic process. Interestingly, the temperature of the linewidth maximum varied with sequence indicating that the thermodynamics of TpA base dynamics are also sequence dependent. In one example, neither a T preceding nor an A trailing the TpA step was required for base dynamics. These results show that base dynamics, heretofore observed in only a few isolated sequences, occurs at all TpA steps which are either preceded or followed by a thymine or adenine, respectively, and may be characteristic of all TpA steps in DNA notwithstanding sequence context.     

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.     

NMR and computational characterization of mitomycin cross-linked to adjacent deoxyguanosines in the minor groove of the d(T-A-C-G-T-A).d(T-A-C-G-T-A) duplex

Two-dimensional homonuclear and heteronuclear NMR and minimized potential energy calculations have been combined to define the structure of the antitumor agent mitomycin C (MC) cross-linked to deoxyguanosines on adjacent base pairs in the d(T1-A2-C3-G4-T5-A6).d(T7-A8-C9-G10-T11-A12) duplex. The majority of the mitomycin and nucleic acid protons in the MC-X 6-mer complex have been assigned from through-bond and through-space two-dimensional proton NMR studies in aqueous solution at 5 and 20 degrees C. The C3.G10 and G4.C9 base pairs are intact at the cross-link site and stack on each other in the complex. The amino protons of G4 and G10 resonate at 9.36 and 8.87 ppm and exhibit slow exchange with solvent H2O. The NMR experimental data establish that the mitomycin is cross-linked to the DNA through the amino groups of G4 and G10 and is positioned in the minor groove. The conformation of the cross-link site is defined by a set of NOEs between the mitomycin H1" and H2" protons and the nucleic acid imino and amino protons of G4 and the H2 proton of A8 and another set of NOEs between the mitomycin geminal H10" protons and the nucleic acid imino and amino protons of G10 and the H2 proton of A2. Several phosphorus resonances of the d(T-A-C-G-T-A) duplex shift dramatically on mitomycin cross-link formation and have been assigned from proton-detected phosphorus-proton two-dimensional correlation experiments. The proton chemical shifts and NOEs establish fraying at the ends of the d(T-A-C-G-T-A) duplex, and this feature is retained on mitomycin cross-link formation. The base-base and base-sugar NOEs exhibit similar patterns for symmetry-related steps on the two nucleic acid strands in the MC-X 6-mer complex, while the proton and phosphorus chemical shifts are dramatically perturbed at the G10-T11 step on cross-link formation. The NMR distance constraints have been included in minimized potential energy computations on the MC-X 6-mer complex. These computations were undertaken with the nonplanar five-membered ring of mitomycin in each of two pucker orientations. The resulting low-energy structures MX1 and MX2 have the mitomycin cross-linked in a widened minor groove with the chromophore ring system in the vicinity of the G10-T11 step on one of the two strands in the duplex.(ABSTRACT TRUNCATED AT 400 WORDS)     

Proton NMR study of the [d(ACGTATACGT)]2-2echinomycin complex: conformational changes between echinomycin binding sites.

The interactions of echinomycin and the DNA decamer [d(ACGTATACGT)]2 were studied by proton NMR. Echinomycin binds cooperatively as a bisintercalator at the CpG steps. The terminal A.T base pairs are Hoogsteen base paired, but none of the four central A.T base pairs are Hoogsteen base paired. However, binding of the drug induces unwinding of the DNA which is propagated to the central ApT step. All four central A.T base pairs are destabilized relative to those in the free DNA. Furthermore, based on these and other results from our laboratory, we conclude that the formation of stable Hoogsteen base pairs may not be the relevant structural change in vivo. The structural changes propagated between adjacent ACGT binding sites are the unwinding of the duplex and destabilization of the base pairing between binding sites.     

Solution structure of [d(GCGTATACGC)]2.

The solution structure of the alternating pyrimidine-purine DNA duplex [d(GCGTATACGC)]2 has been determined using two-dimensional nuclear magnetic resonance techniques and distance geometry methods. Backbone distance constraints derived from experimental nuclear Overhauser enhancement and J-coupling torsion angle constraints were required to adequately define the conformation of the inter-residue backbone linkages and to avoid underwinding of the duplex. The distance geometry structures were further refined by back-calculation of the two-dimensional nuclear Overhauser enhancement spectra to correct spin-diffusion distance errors. Fifteen final structures for [d(GCGTATACGC)]2 were generated from the refined experimental distance bounds. These structures all exhibit fully wound B-form geometry with small penalty values (< 1.5 A) against the distance bounds and small pair-wise root-mean-square deviation values (typically 0.6 A to 1.5 A). The final structures exhibit positive base-pair inclination with respect to the helix axis, a marked alternation in rise and twist, and are shorter and wider than classical fiber B-form DNA. The purines were found to adopt a sugar pucker close to the C-2'-endo conformation while pyrimidine sugars exhibited significantly lower pseudorotation phase angles in the C-1'-exo to C-2'-endo range. The minor groove cross-strand steric clashes at pyrimidine-purine steps that would exist in pure B-DNA are attenuated by an increased rise at these steps (and an increased roll angle at TpA steps). Concomitantly the backbone torsion angles of the pyrimidine moieties have larger gamma values, larger epsilon values, and smaller zeta values than the purines. The structures generated by distance geometry methods were also compared with those obtained from restrained molecular dynamics with empirical force-field potentials. The results indicate that the nuclear magnetic resonance/distance geometry approach alone is capable of elucidating most of the salient structural features of double-stranded helical nucleic acids in solution without resorting to empirical energy potentials and without using any structural assumptions from crystallographic data.     

Intrinsic bending and deformability at the T-A step of CCTTTAAAGG: a comparative analysis of T-A and A-T steps within A-tracts

Introduction of a T-A or pyrimidine-purine step into a straight and rigid A-tract can cause a positive roll deformation that kinks the DNA helix at that step. In CCTTTAAAGG, the central T-A step has an 8.6 degrees bend toward the major groove. We report the structural analysis of CCTTTAAAGG and a comparison with 25 other representative crystal structures from the NDB containing at least four consecutive A or T bases. On average, more local bending occurs at the disruptive T-A step (8.21 degrees ) than at an A-T step (5.71 degrees ). In addition, A-tracts containing an A-T step are more bent than are pure A-tracts, and hence A-A and A-T steps are not equivalent. All T-A steps examined exhibit positive roll, bending towards the major groove, while A-T steps display negative roll and bend slightly towards the minor groove. This illustrates how inherent negative and positive roll are, respectively, at A-T and T-A steps within A-tracts. T-A steps are more deformable, showing larger and more variable deformations of minor groove width, rise, cup, twist, and buckle. Standard deviations of twist, rise, and cup for T-A steps are 6.66 degrees, 0.55 A, and 15.90 degrees, versus 2.28 degrees, 0.21 A, and 2.99 degrees for A-T steps. Packing constraints determine which local values of these helical parameters an individual T-A step will adopt. For instance, with CCTTTAAAGG and three isomorphous structures, CGATTAATCG, CGATATATCG, and CGATCGATCG, crystal packing forces lead to a series of correlated changes: widened minor groove, large slide, low twist, and large rise. The difference in helical parameters between A-T steps lying within A-tracts, versus A-T steps within alternating AT sequences, demonstrates the importance of neighboring steps on the conformation of a given dinucleotide step.     

The solution conformation of a carbocyclic analog of the Dickerson-Drew dodecamer: comparison with its own X-ray structure and that of the NMR structure of the native counterpart

The NMR conformation of a carbocyclic analog of the Dickerson-Drew dodecamer [d(CGC-GAAT*T*CGCG)]2 containing 6'-alpha-Me carbocyclic thymidines (T*) has been determined and compared with that of its X-ray structure. The solution structure of the 6'-alpha-Me carbocyclic thymidine modified duplex has also been compared with the solution structure of the corresponding unmodified Dickerson-Drew duplex solved by us under the same experimental conditions. The NMR structures have been based on 24 experimental distance and torsion constraints per residue for [d(CGCGAAT*T*CGCG)]2 (1) and on 21 constraints per residue for the natural counterpart. In general, both final NMR structures are more close to the B-type DNA. The cyclopentane moieties of the carbocyclic thymidine residues adopt C1'-exo B-DNA type puckers (the phase angles P = 136-139 degrees and the puckering amplitudes psi = 36-37 degrees) that are close to their previously published crystal C1'-exo or C2'-endo puckers. The main differences between the two NMR structures are for beta(T*8) and epsilon, xi(T*7) backbone torsions (27-50 degrees ), for basepair twist for the 7-8 and 8-9 basepair steps (5-6 degrees), tilt for the 8-9 step (7 degrees), roll for the 7-8 step (7 degrees), shift for the 7-8 step (0.9A) and slide for the 9-10 step (0.6A). The relatively small deviations of helical structure parameters lead to structural isomorphism of these duplexes in aqueous solutions (atomic RMSD = 1.0A). The difference of the minor groove widths (less than 0.7A) in the core part of the modified duplex in comparison with the native one is much smaller than the difference between the X-ray structures of these duplexes. A detailed comparison of NMR and X-ray structure parameters showed significant monotonic differences (0.9-2.5A) for all basepair slides in both duplexes. Deviations between NMR and X-ray structure parameters for the modified duplex were also found for basepair tilt of the 4-5 step (13 degrees), rolls for the 8-9 and 10-11 steps (16 and 19 degrees), twist of the 3-4 step (8 degrees) and shift of the 9-10 step (0.9A).     

The solution structure of the intramolecular photoproduct of d(TpA) derived with the use of NMR and a combination of distance geometry and molecular dynamics.

One and two dimensional NMR techniques have been used together with molecular modelling to obtain the solution structure for the photoproduct d(TpA)*. The NMR data confirm that the cyclobutane linkage is formed between the bonds thymine C6-C5 and adenine C5-C6. The 2D NOE data are used as constraints in a distance geometry calculation. The structures obtained show a trans-syn cyclobutane linkage and the glycosidic angles are SYN and ANTI for thymidine and deoxyadenosine, respectively. The coupling constant data are used to check the backbone torsion angles of the obtained structures. Typical torsion angles are a gamma+ and beta t for the deoxyadenosine residue. A free molecular dynamics simulation of a trans-syn d(TpA) photoproduct confirmed all these structural characteristics.     

Slow motion in the CAA*TTG sequence of a DNA decamer duplex studied by NMR

In DNA duplexes, pyrimidine-purine steps are believed to be flexible or conformationally unstable. Indeed, several DNA crystal structures exhibit a multitude of conformations for CpA*TpG steps. The question arises of whether this structural flexibility is accompanied by dynamical flexibility, i.e., a question pertaining to the energy barrier between conformations. Except for TpA steps, slow motions on the microsecond-to-millisecond time scale have not been detected in duplexes until now. In the present study, such slow motion was investigated by 1H, 13C, and 15N NMR relaxation measurements on a DNA decamer d(CATTTGCATC)*d(GATGCAAATG). The DNA decamer was enriched with 15% 13C and 98% 15N isotopes for each adenosine and guanosine residue. Three lines of evidence support the notion of slow motion in the CAA*TTG moiety. Analysis of (15)N relaxation showed that the order parameter, S2, of guanosine imino NH groups was about 0.8, similar to that of CH groups for this oligomer. The strong temperature dependence of guanosine NH S2 in the CAA*TTG sequence indicated the presence of a large-amplitude motion. Signals of adenosine H8 protons in the CAA*TTG sequence were broadened in 2D 1H NOESY spectra, which also suggested the existence of slow motion. As well as being smaller than for other adenine residues, the 1H T2 values exhibited a magnetic field strength dependence for all adenosine H8 signals in the ATTTG*CAAAT region, suggesting slow motions more pronounced at the first adenosine in the CAA*TTG sequence but extending over the CAAAT*ATTTG region. This phenomenon was further examined by the pulse field strength dependence of the 1H, 13C, and 15N T1rho values. 1H and 13C T1rho values showed a pulse field strength dependence, but 15N T1rho did not. Assuming a two-site exchange process, an exchange time constant of 20-300 micros was estimated for the first adenosine in the CAA sequence. The exact nature of this motion remains unknown.     

High-resolution crystal structure of the intramolecular d(TpA) thymine-adenine photoadduct and its mechanistic implications

A high-resolution crystal structure is reported for d(TpA)*, the intramolecular thymine–adenine photoadduct that is produced by direct ultraviolet excitation of the dinucleoside monophosphate d(TpA). It confirms the presence of a central 1,3-diazacyclooctatriene ring linking the remnants of the T and A bases, as previously deduced from heteronuclear NMR measurements by Zhao et al. (The structure of d(TpA)*, the major photoproduct of thymidylyl-(3′-5′)-deoxyadenosine. Nucleic Acids Res., 1996, 24, 1554–1560). Within the crystal, the d(TpA)* molecules exist as zwitterions with a protonated amidine fragment of the eight-membered ring neutralizing the charge of the internucleotide phosphate monoanion. The absolute configuration at the original thymine C5 and C6 atoms is determined as 5S,6R. This is consistent with d(TpA)* arising by valence isomerization of a precursor cyclobutane photoproduct with cis–syn stereochemistry that is generated by [2 + 2] photoaddition of the thymine 5,6-double bond across the C6 and C5 positions of adenine. This mode of photoaddition should be favoured by the stacked conformation of adjacent T and A bases in B-form DNA. It is probable that the primary photoreaction is mechanistically analogous to pyrimidine dimerization despite having a much lower quantum yield.     

Sequence-dependent variation in DNA minor groove width dictates orientational preference of Hoechst 33258 in A-tract recognition: solution NMR structure of the 2:1 complex with d(CTTTTGCAAAAG)(2)

The solution structure of the dodecamer duplex d(CTTTTGCAAAAG)₂ and its 2:1 complex with the bis-benzimidazole Hoechst 33258 has been investigated by NMR and NOE-restrained molecular dynamics (rMD) simulations. Drug molecules are bound in each of the two A-tracts with the bulky N-methylpiperazine ring of each drug located close to the central TG (CA) step, binding essentially to the narrow minor groove of each A-tract. MD simulations over 1 ns, using an explicit solvation model, reveal time-averaged sequence-dependent narrowing of the minor groove from the 3′-end towards the 5′-end of each TTTT sequence. Distinct junctions at the TpG (CpA) steps, characterised by large positive roll, low helical and propeller twists and rapid AT base pair opening rates, add to the widening of the groove at these sites and appear to account for the bound orientation of the two drug molecules with the N-methylpiperazine ring binding in the wider part of the groove close to the junctions. Comparisons between the free DNA structure and the 2:1 complex (heavy atom RMSD 1.55 Å) reveal that these sequence-dependent features persist in both structures. NMR studies of the sequence d(GAAAAGCTTTTC)₂, in which the A-tracts have been inverted with the elimination of the TpG junctions, results in loss of orientational specificity of Hoechst 33258 and formation of multiple bound species in solution, consistent with the drug binding in a number of different orientations.     

Anomalous structure and properties of poly (dA).poly(dT). Computer simulation of the polynucleotide structure with the spine of hydration in the minor groove.

The results of the search for low-energy conformations of poly(dA).poly(dT) and of the poly(dA).poly(dT) "complex" with the spine of hydration similar to that found by Dickerson and co-workers (Kopka, M.L., Fratini, A.V., Drew, H.R. and Dickerson, R.E. (1983) J. Mol. Biol. 163, 129-146) in the minor groove of the CGCGAATTCGCG crystals are described. It is shown that the existence of such a spine in the minor groove of poly(dA).poly(dT) is energetically favourable. Moreover, the spine of hydration makes the polynucleotide conformation similar to the poly(dA).poly(dT) structure in fibers and to the conformation of the central part of CGCGAATTCGCG in crystals; it also acquires features characteristic of the structure of poly(dA).poly(dT) and DNA oligo(dA)-tracts in solution. It is shown that the existence of the TpA step in conformations characteristic of the poly(dA).poly(dT) complex with the spine of hydration is energetically unfavourable (in contrast to the ApT step) and therefore this step should result in destabilization of the spine of hydration in the DNA minor groove. Thus, it appears that the spine of hydration as described by Dickerson and co-workers is unlikely to exist in the poly d(A-T).poly d(A-T) structure. The data obtained permit us to interpret a large body of experimental facts concerning the unusual structure and properties of poly(dA).poly(dT) and oligo(dA)-tracts in DNA both in fibers and in solution. The results provide evidence of the existence of the minor groove spine of hydration both in fibers and in solution on A/T tracts of DNA which do not contain the TpA step. The spine plays an active role in the formation of the anomalous conformation of these tracts.     

Further studies on telestability in DNA. The synthesis and characterization of the duplex block polymers d(C20A10) - d(T10G20) and d(C20A15) - d(T15G20).

The synthesis and characterization of the duplex block polymers d(C20A10) - d(T10G20) and d(C20A15) - d(T15G20) are described. Thermal denaturation studies on these DNAs in the absence and presence of actinomycin, which binds only to the GC portions of these molecules, have confirmed and extended our previous observation that the properties of one region of a DNA can be influenced (telestabilized) by a remote region. In addition, the large scale synthesis of d(C15A15) - d(T15G15) is described.