Circular dichroism spectra of DNA oligomers show that short interior stretches of C.C+ base pairs do not form in duplexes with A.T base pairs

Circular dichroism (CD) experiments were carried out on a series of DNA oligomers to determine if short internal stretches of protonated cytosine-cytosine (C.C+) base pairs could coexist with adenine-thymine (A.T) base pairs. (1) C.C+ base pairs did form in the absence of A.T base pairs in the individual oligomers d(AACC)5 and d(CCTT)5, as indicated by the appearance of a long-wavelength CD band centered at 282-284 nm, when the pH was lowered to 6 or 5 at 0.5 M Na+. A comparison of measured with calculated spectra showed that d(CCTT)5 at pH 5, 0.5 M Na+, 20 degrees C, likely adopted a structure with a central core of stacked C.C+ base pairs and looped-out thymines. Under the same conditions, it appeared that C.C+ base pairs also formed in d(AACC)5, but with the adenines remaining intrahelical. Each of these oligomers showed a cooperative transition for formation of C.C+ base pairs as the temperature was lowered, with C.C+ base pairs forming at a higher temperature in d(CCTT)5 than in d(AACC)5. A.T base formed in equimolar mixtures of d(AACC)5 plus d(CCTT)5 as monitored by an increase in the negative magnitude of the 250-nm CD band. However, a large increase did not appear at about 285 nm in CD spectra of the mixtures, showing that there were no stacked C.C+ base pairs in the d(AACC)5.d(CCTT)5 duplex even though they formed under the same conditions in the individual strands. Thus, in this duplex, A.T base pairs prevented the formation of neighboring internal C.C+ base pairs. (2) CD measurements were also made of d(A10C4T10).(ABSTRACT TRUNCATED AT 250 WORDS)     

Circular dichroism measurements show that C.C+ base pairs can coexist with A.T base pairs between antiparallel strands of an oligodeoxynucleotide double-helix.

We have studied the coil-to-helix transition of the DNA oligomer d(C4A4T4C4), using circular dichroism measurements to monitor the formation of A.T base pairs within the central self-complementary A4T4 region and the formation of protonated C.C+ base pairs at the ends of the oligomer. We found that both A.T and C.C+ base pairs formed in a coordinated fashion as the temperature and pH were lowered. The CD data of the helix form of the oligomer were consistent with the presence of paired oligomers, but not with hairpin loops. The pKa for formation of C.C+ base pairs between the C4 ends of the oligomer was higher than the pKa for formation of C.C+ base pairs in d(C8), indicating that the formation of C.C+ base pairs in the oligomer was influenced by the presence of a paired A4T4 region. We conclude that A.T and C.C+ base pairs coexist in the self-complex of the oligomer and, therefore, that C.C+ base pairs can form between antiparallel DNA strands.     

Photochemical demonstration of stacked C.C+ base pairs in a novel DNA secondary structure

The secondary structure of the alternating polydeoxynucleotide sequence poly[d(C-T)] was studied as a function of pH by ultraviolet absorbance and circular dichroism spectroscopy and by the analysis of UV-induced photoproducts. As the pH was lowered, poly[d(C-T)] underwent a conformational transition that was characterized by changes in the long-wavelength region (280-320 nm) of the CD spectrum. These changes have previously been interpreted as evidence for the formation of a core of stacked, protonated C X C+ base pairs in a double-helical complex of poly[d(C-T)], with the thymidyl residues being looped out into the solvent [Gray, D. M., Vaughan, M., Ratliff, R. L., & Hayes, F. N. (1980) Nucleic Acids Res. 8, 3695-3707]. In the present work, poly[d(C-T)] was labeled with [U-14C]cytosine and [methyl-3H]thymine and irradiated at pH values both above and below the conformational transition point (monitored by CD spectroscopy). The distribution of radioactivity in uracil means value of uracil dimers, uracil means value of thymine dimers (the deamination products of cytosine means value of cytosine and cytosine means value of thymine dimers, respectively), and thymine-means value of thymine dimers was then determined. As the pH was decreased, we found an increase in the yield of uracil means value of uracil dimers and a decrease in the yield of uracil means value of thymine dimers, which occurred concomitantly with the change in the CD spectrum.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Ff gene 5 protein has a high binding affinity for single-stranded phosphorothioate DNA

The gene 5 protein (g5p) of Ff bacteriophages is a well-studied model ssDNA-binding protein that binds cooperatively to the Ff ssDNA genome and single-stranded polynucleotides. Its affinity, K omega (the intrinsic binding constant times a cooperativity factor), can differ by several orders of magnitude for ssDNAs of different nearest-neighbor base compositions [Mou, T. C., Gray, C. W., and Gray, D. M. (1999) Biophys. J. 76, 1537-1551]. We found that the DNA backbone can also dramatically affect the binding affinity. The K omega for binding phosphorothioate-modified S-d(A)(36) was >300-fold higher than for binding unmodified P-d(A)(36) at 0.2 M NaCl. CD titrations showed that g5p bound phosphorothioate-modified oligomers with the same stoichiometry as unmodified oligomers. The CD spectrum of S-d(A)(36) underwent the same qualitative change upon protein binding as did the spectrum of unmodified DNA, and the phosphorothioate-modified DNA appeared to bind in the normal g5p binding site. Oligomers of d(A)(36) with different proportions of phosphorothioate nucleotides had binding affinities and CD perturbations intermediate to those of the fully modified and unmodified sequences. The influence of phosphorothioation on binding affinity was nearly proportional to the extent of the modification, with a small nearest-neighbor dependence. These and other results using d(ACC)(12) oligomers and mutant proteins indicated that the increased binding affinity of g5p for phosphorothioate DNA was not a polyelectrolyte effect and probably was not an effect due to the altered nucleic acid structure, but was more likely a general effect of the properties of the sulfur in the context of the phosphorothioate group.     

Conformations of duplex structures formed by oligodeoxynucleotides covalently linked to the intercalator 2-methoxy-6-chloro-9-aminoacridine

A family of covalent complexes between oligonucleotides and derivatives of the intercalating agent 9-amino acridine has been synthesized (Asseline, U., Thuong, N.T. and Helene, C. (1983) C.R.Acad. Sci. (Paris) 297 (III), 369-372) and studied (Lancelot, G., Asseline, U., Thuong, N.T., and Helene, C. (1985) Biochemistry 24, 2521-2529; Lancelot, G., Asseline, U., Thuong, N.T., and Helene, C. (1985) J. Biomol. Str. Dyn. 3, 913-921) with a view to understand nucleic acid-nucleic acid recognition. In order to understand the nature of interactions between the intercalator and the oligonucleotides in such complexes and the sensitivity of such interactions to the polymorphic form of the DNA, we have carried out molecular mechanics simulations on duplex deoxyoligonucleotides d(A)6.d(T)6 (A and B forms) and d(TATC).d(GATA) (B form) covalently bound to 2-methoxy-6-chloro-9-aminoacridine through a pentamethylene linker chain. Structures in which the acridine derivative is end stacked (at the 3' and 5' ends) and in which the dye is intercalated between the terminal base pairs (at both the ends) and between second and third base pairs from the 3' end are all of reasonably low energy in both A and B forms of DNA. Our studies on 3' end complexes find that in the B form, intercalation of the dye between the second and third base pairs is preferred over the other two modes of binding, while in the A form, intercalation between the terminal base pairs is preferred. In the 5' end A and B form complexes, outside stacking and intercalation between the terminal base pairs are preferred, respectively. Our calculations suggest the possibility that the presence of the dye attached covalently to the DNA can induce conformational transitions in the DNA. For example, intercalation of the dye two base pairs from the end could induce an A----B transition.     

Thermodynamics of triple helix formation: spectrophotometric studies on the d(A)10.2d(T)10 and d(C+3T4C+3).d(G3A4G3).d(C3T4C3) triple helices.

We have stabilized the d(A)10.2d(T)10 and d(C+LT4C+3).d(G3A4G3).d(C3T4C3) triple helices with either NaCl or MgCl2 at pH 5.5. UV mixing curves demonstrate a 1:2 stoichiometry of purine to pyrimidine strands under the appropriate conditions of pH and ionic strength. Circular dichroic titrations suggest a possible sequence-independent spectral signature for triplex formation. Thermal denaturation profiles indicate the initial loss of the third strand followed by dissociation of the underlying duplex with increasing temperature. Depending on the base sequence and ionic conditions, the binding affinity of the third strand for the duplex at 25 degrees C is two to five orders of magnitude lower than that of the two strands forming the duplex. Thermodynamic parameters for triplex formation were determined for both sequences in the presence of 50 mM MgCl2 and/or 2.0 M NaCl. Hoogsteen base pairs are 0.22-0.64 kcal/mole less stable than Watson-Crick base pairs, depending on ionic conditions and base composition. C+.G and T.A Hoogsteen base pairs appear to have similar stability in the presence of Mg2+ ions at low pH.     

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.     

N(4)C-ethyl-N(4)C cross-linked DNA: synthesis and characterization of duplexes with interstrand cross-links of different orientations.

The preparation and physical properties of short DNA duplexes that contain a N(4)C-ethyl-N(4)C interstrand cross-link are described. Duplexes that contain an interstrand cross-link between mismatched C-C residues and duplexes in which the C residues of a -CG- or -GC- step are linked to give "staggered" interstrand cross-links were prepared using a novel N(4)C-ethyl-N(4)C phosphoramidite reagent. Duplexes with the C-C mismatch cross-link have UV thermal transition temperatures that are 25 degrees C higher than the melting temperatures of control duplexes in which the cross-link is replaced with a G-C base pair. It appears that this cross-link stabilizes adjacent base pairs and does not perturb the structure of the helix, a conclusion that is supported by the CD spectrum of this duplex and by molecular models. An even higher level of stabilization, 49 degrees C, is seen with the duplex that contains a -CG- staggered cross-link. Molecular models suggest that this cross-link may induce propeller twisting in the cross-linked base pairs, and the CD spectrum of this duplex exhibits an unusual negative band at 298 nm, although the remainder of the spectrum is similar to that of B-form DNA. Mismatched C-C or -CG- staggered cross-linked duplexes that have complementary overhanging ends can undergo self-ligation catalyzed by T4 DNA ligase. Analysis of the ligated oligomers by nondenaturing polyacrylamide gel electrophoresis shows that the resulting oligomers migrate in a manner similar to that of a mixture of non-cross-linked control oligomers and suggests that these cross-links do not result in significant bending of the helix. However, the orientation of the staggered cross-link can have a significant effect on the structure and stability of the cross-linked duplex. Thus, the thermal stability of the duplex that contains a -GC- staggered cross-link is 10 degrees C lower than the melting temperature of the control, non-cross-linked duplex. Unlike the -CG- staggered cross-link, in which the cross-linked base pairs can still maintain hydrogen bond contacts, molecular models suggest that formation of the -GC- staggered cross-link disrupts hydrogen bonding and may also perturb adjacent base pairs leading to an overall reduction in helix stability. Duplexes with specifically positioned and oriented cross-links can be used as substrates to study DNA repair mechanisms.     

NMR studies of pH-dependent conformational polymorphism of alternating (C-T)n sequences.

Alternating (C-T)n sequences are involved in the H-DNA structure associated with (GA)n.(CT)n sequences. Low pH values facilitate H-DNA formation. We have undertaken a detailed analysis of the structural consequences of the (C-T)n sequence as a function of pH. The structures of three DNA oligonucleotides, d(CT)4, d(TC)4 and d(TC)15, have been studied by NMR. We found that their conformations are polymorphic and pH dependent. There are at least three major conformational species: an antiparallel-stranded (APS) duplex with entirely C:T base pairs at pH 7, an antiparallel-stranded (APS) duplex with entirely C+:T base pairs at pH 3, and a possible parallel-stranded (PS) duplex with C+:C and T:T base pairs near pH 5. In the intermediate pH range, the APS duplex may have varying numbers of C+:T and C:T base pairs, and there may be a fast exchange going on between APS duplex species involving these two kinds of base pairs. However, the transition between the APS and PS duplexes is slow. Structural refinement of the two octamers, d(TC)4 and d(CT)4, at pH = 6.9 and pH = 3 using 2D-NOE data suggests that the molecules are likely in the duplex form at 5 degrees C. We lack evidence that the structure at pH 3 is a PS structure with T nucleotides residing in the exterior of the helix. Titration of the longer oligonucleotide, d(TC)15, showed a prominent pKa of approximately 6, approaching the value of 7.0 obtained from the titration of poly-(dC).     

The thermal stability of DNA fragments with tandem mismatches at a d(CXYG).d(CY'X'G) site.

Temperature-Gradient Gel Electrophoresis (TGGE) was employed to determine the thermal stabilities of 28 DNA fragments, 373 bp long, with two adjacent mismatched base pairs, and eight DNAs with Watson-Crick base pairs at the same positions. Heteroduplex DNAs containing two adjacent mismatches were formed by melting and reannealing pairs of homologous 373 bp DNA fragments differing by two adjacent base pairs. Product DNAs were separated based on their thermal stability by parallel and perpendicular TGGE. The polyacrylamide gel contained 3.36 M urea and 19.2 % formamide to lower the DNA melting temperatures. The order of stability was determined in the sequence context d(CXYG).d(CY'X'G) where X.X' and Y.Y" represent the mismatched or Watson-Crick base pairs. The identity of the mismatched bases and their stacking interactions influence DNA stability. Mobility transition melting temperatures (T u) of the DNAs with adjacent mismatches were 1.0-3.6 degrees C (+/-0.2 degree C) lower than the homoduplex DNA with the d(CCAG).d(CTGG) sequence. Two adjacent G.A pairs, d(CGAG).d(CGAG), created a more stable DNA than DNAs with Watson-Crick A.T pairs at the same sites. The d(GA).d(GA) sequence is estimated to be 0.4 (+/-30%) kcal/mol more stable in free energy than d(AA).d(TT) base pairs. This result confirms the unusual stability of the d(GA).d(GA) sequence previously observed in DNA oligomers. All other DNAs with adjacent mismatched base pairs were less stable than Watson-Crick homoduplex DNAs. Their relative stabilities followed an order expected from previous results on single mismatches. Two homoduplex DNAs with identical nearest neighbor sequences but different next-nearest neighbor sequences had a small but reproducible difference in T u value. This result indicates that sequence dependent next neighbor stacking interactions influence DNA stability.     

Effects of adduct formation derived from ethylene dibromide on DNA conformation.

Spectral properties of DNA oligomers containing the single modified guanine, S-[2-(N7-guanyl)ethyl]-glutathione, the major adduct derived from 1,2-dibromoethane, were investigated using UV, CD, and NMR. Two palindromic hexamers, d(ATGCAT) and d(ATCGAT), did not form a duplex with guanine bases modified. When the non self-complementary heptamer, d(CATGCCT), was modified at the single guanine, it formed a duplex with its normal complement d(AGGCATG), although the melting temperature was lowered. However, no duplex formation was observed when a non complementary base other than cytosine was placed in d(AGGXATG), suggesting that non Watson-Crick type base pairs are not stabilized by formation of this adduct.     

Unusual DNA conformation at low pH revealed by NMR: parallel-stranded DNA duplex with homo base pairs.

We have investigated the conformational potentials of several DNA oligonucleotides containing sequences related to 5'-CGA in neutral pH and low pH (< 5.0) conditions. One-dimensional proton NMR spectra show that d(CGATCG), d(TCGATCGA), and d(CGATCGATCG) exhibit new sets of resonances at low pH (approximately 3.8-4.4), when compared to those from the neutral pH samples. The low pH form and the neutral pH form are in slow equilibrium. Analyses of the data suggest that these sequences under low pH conditions adopt structures distinct from B-DNA. Two-dimensional nuclear Overhauser effect spectroscopy (2D NOESY) data from the DNA hexamer d(CGATCG) of the neutral and low pH samples were used to analyze their respective structures in solution. An iterative NOE spectral-driven refinement procedure, SPEDREF [Robinson, H., & Wang, A. H.-J. (1992) Biochemistry 31, 3524-3533], was used to show that the neutral pH structure is close to canonical B-DNA. In contrast, analysis of the low pH form using the 2D NOESY data suggests that its structure is consistent with a right-handed parallel-stranded (PS) double helix with symmetrical non-Watson-Crick (C+:C, G:G, A:A, T:T) homo base pairs. Supporting evidence for the PS helix includes the asymmetric inversion-recovery relaxation times associated with the two ends of the helix. The structure is favored by the 5'-CGA sequence in which the cytosines provide the C+:C pairing for the nucleation step and the GpA step is significantly stabilized by the interstrand G-A stacking interactions.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effect of the methyl group on DNA bending and curvature: structure of d(GA4U4C)2 in solution

NMR studies on d(GA4T4C)2 and d(GT4A4C)2 indicated two important factors that contribute to intrinsic DNA bending in polymers containing A/T tracts [Sarma, M.H., et al. (1988) Biochemistry 27, 3423; Gupta, G., et al. (1988) Biochemistry 27, 7909]. They are (i) propeller-twisted A.T pairs with associated bifurcated H bonds inside the A/T tract and (ii) the base sequence that joins the two neighboring A/T tracts. As an extension of our bending project, we carried out quantitative NMR studies on the decamer d(GA4U4C)2, a structural analogue of d(GA4T4C)2, to examine the effect of the methyl group on DNA bending. On the basis of quantitative NMR analysis, we arrive at the following results. (i) The decamer d(GA4U4C)2 adopts the gross morphology of a right-handed B-DNA duplex with A and U nucleotides belonging to C2'-endo,anti domain. (ii) A.U pairs are propeller twisted and hence can result in an array of interstrand bifurcated H bonds involving N6 of A and O4 of U (one base pair apart) inside the A/U tract. (iii) The orientations of A and U with respect to the long axis of the molecule are different; as a result, at the A5-U6 sequence that joins the two A/U tracts, two neighboring frames of reference do not exactly coincide in space and a junction is created at A5-U6. (iv) Inside the A/U tract, intrastrand stacking is more compact (average separation between secessive base planes being 3.2 A) than at the A5-U6 junction, where average separation between the base planes of A5 and U6 is 3.6 A.(ABSTRACT TRUNCATED AT 250 WORDS)     

Base sequence criteria and Cartesian coordinates for stable B/Z and B/Z/B junctions in relaxed DNA.

It seems increasingly evident that if the Z form of DNA exists in the genome it must exist as short sections of alternating pyrimidine-purine sequences in the midst of very long sections of B-form DNA. We have determined the minimum length of a string of alternating CG base pairs that can go into the Z form in the middle of a long B form. Self-complimentary oligomers of the form T(M)(CG)(N)A(M) were synthesized. The conformation of the resulting duplex was determined in 6M aqueous NaCl solution by Raman scattering. We have found that 12 alternating CG base pairs is the minimum length required to form a stable Z form of DNA inside of a long B form section. Only the 4 center CG base pairs go into the Z form. These 4 CG base pairs in the Z form are flanked on each side by 4 CG base pairs in a non-Z (probably B) form as well as the ..TT.. ..AA.. sequences in the B form. We propose a model of the B/Z junction in which the double helix flips directly from the B form to the Z form so that there are no base pairs in the junction. In this model the B form is nucleated in the AT base pairs on each end and is propagated into the CG base pairs in the center. This model is supported by isotopic H/D exchange experiments that shows that the H/D exchange of the non-Z form CG base pairs is highly retarded and indicates that they remain in the B form. A Thermodynamic analysis of the concentration dependence of the melting point of the duplexes in both low and high salt, supports our model and rules out the possibility of hairpin formation. The enthalpy for the formation of a B/Z junction is determined to be about +16 kcal/junction. A comparison of these results with recent results on B/Z junctions in super-coiled DNA is given. Molecular modeling calculations permit us to obtain values for the coordinates and torsional angles of the oligomers showing both B/Z and B/Z/B junctions. The Cartesian coordinates for these oligomers as well as stereo figures of these models in color are available from the authors.     

Proton exchange in DNA-luzopeptin and DNA-echinomycin bisintercalation complexes: rates and processes of base-pair opening.

Imino proton exchange studies are reported on the complexes formed by bisintercalation of luzopeptin around the two central A.T pairs of the d(CCCATGGG) and d(AGCATGCT) duplexes and of echinomycin around the two central C.G pairs of the d(AAACGTTT) and d(CCAAACGTTTGG) duplexes. The depsipeptide backbone of the drugs occupies the minor groove of the complexes at the bisintercalation site. The exchange time of the amide protons of the depsipeptide rings provides a lower estimate of the complex lifetime: 20 min at 15 degrees C for the echinomycin complexes and 4 days at 45 degrees C for the luzopeptin complexes. The exchange time of imino protons is always shorter than the complex lifetime. Hence, base pairs open even within the complexed oligomers. For the two base pairs sandwiched between the aromatic rings of the drug, the base-pair lifetime is strongly increased, and the dissociation constant is correspondingly reduced. Hence, the lifetime of the open state is unchanged. This suggests similar open states in the free duplex and in the complex. In contrast to the sandwiched base pairs, the base pairs flanking the intercalation site are not stabilized in the complex. Thus, the action of the bisintercalating drug may be compared to a vise clamping the inner base pairs. Analysis suggests that base-pair opening may require prior unwinding or bending of the DNA duplex.     

Influence of sequence context and length on the structure and stability of triplet repeat DNA oligomers

Genetic expansion diseases have been linked to the properties of triplet repeat DNA sequences during replication. The most common triplet repeats associated with such diseases are CAG, CCG, CGG, and CTG. It has been suggested that gene expansion occurs as a result of hairpin formation of long stretches of these sequences on the leading daughter strand synthesized during DNA replication [Gellibolian, R., Bacolla, A., and Wells, R. D. (1997) J. Biol. Chem. 272, 16793-7]. To test the biophysical basis for this model, oligonucleotides of general sequence (CNG)(n), where N = A, C, G, or T and n = 4, 5, 10, 15, or 25, were synthesized and characterized by circular dichroism (CD) spectropolarimetry, optical melting studies, and differential scanning calorimetry (DSC). The goal of these studies was to evaluate the influence of sequence context and oligomer length on their secondary structures and stabilities. The results indicate that all single oligomers, even those as short as 12 nucleotides, form stable hairpin structures at 25 degrees C. Such hairpins are characterized by the presence of N:N mismatched base pairs sandwiched between G:C base pairs in the stems and loops of three to four unpaired bases. Thermodynamic analysis of these structures reveals that their stabilities are influenced by both the sequence of the particular oligomer and its length. Specifically, the stability order of CGG > CTG > CAG > CCG was observed. In addition, longer oligomers were found to be more stable than shorter oligomers of the same sequence. However, a stability plateau above 45 nucleotides suggests that the length dependence reaches a maximum value where the stability of the G:C base pairs can no longer compensate the instability of the N:N mismatches in the stems of the hairpins. The results are discussed in terms of the above model proposed for gene expansion.     

The intrinsic structure and stability of out-of-alternation base pairs in Z-DNA.

Alternating pyrimidine-purine sequences typically form Z-DNA, with the pyrimidines in the anti and purines in the syn conformations. The observation that dC and dT nucleotides can also adopt the syn conformation (i.e. the nucleotides are out-of-alternation) extends the range of sequences that can convert to this left-handed form of DNA. Here, we study the effects of placing two adjacent d(G*C) base pairs as opposed to a single d(G*C) base pair or two d(A*T) base pairs out-of-alternation by comparing the structure of d(m5CGGCm5CG)2with the previously published structures of d(m5CGGGm5CG)*d(m5CGCCm5CG) and d(m5CGATm5CG)2. A high buckle and loss of stacking interactions are observed as intrinsic properties of the out-of-alternation base pairs regardless of sequence and the context of the dinucleotide. From solution titrations, we find that the destabilizing effect of out-of-alternation d(G*C) base pairs are identical whether these base pairs are adjacent or isolated. We can therefore conclude that it is these intrinsic distortions in the structure of the base pairs and not neighboring effects that account for the inability of out-of-alternation base pairs to adopt the left-handed Z conformation.     

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.