The molecular structure of Okazaki fragment r(CGCA)d(AAAAAGCG):d(CGCTTTTTTGCG) in solution

The hetero duplex molecule, r(CGCA)d(AAAAAGCG):d(CGCTTTTTTGCG) which corresponds to Okazaki fragment was synthesized and its molecular structure has been analyzed by NMR study. The RNA strand of RNA-DNA hybrid region adopts A-form and DNA strand of the same region deviates from the standard B-form. The conformation of DNA-DNA duplex segment belongs to B-form. The hybrid-DNA duplex junction shows a structural discontinuities, A-B junction. The same conformational characteristic of oligo(dA): oligo(dT) tract as that of DNA oligomer which has same base sequence has been observed.     

Conformational analysis of d(C3G3), a B-family duplex in solution

NMR and circular dichroism studies of the duplex formed by the self-complementary DNA hexanucleotide d(C3G3) indicate that it is a B-type structure but differs from standard B-form. An analysis of NMR coupling constants within the deoxyribose moieties yields a 70% or greater contribution from pseudorotation phase angles corresponding to the C3'-exo conformation, a conformation similar to the C2'-endo conformation associated with B-form DNA. Intranucleotide interproton distances are consistent with a B-form structure, but some internucleotide distances are intermediate between A- and B-form structures. Circular dichroism spectra have B-form characteristics but also include an unusual negative band at 282 nm. The solution spectroscopic results are in contrast with X-ray crystallographic studies which find A-form structures for similar sequences.     

Structure of d(T)n.d(A)n.d(T)n: the DNA triple helix has B-form geometry with C2'-endo sugar pucker.

The polynucleotide helix d(T)n.d(A)n.d(T)n is the only deoxypolynucleotide triple helix for which a structure has been published, and it is generally assumed as the structural basis for studies of DNA triplexes. The helix has been assigned to an A-form conformation with C3'-endo sugar pucker by Arnott and Selsing [1974; cf. Arnott et al. (1976)]. We show here by infrared spectroscopy in D2O solution that the helix is instead B-form and that the sugar pucker is in the C2'-endo region. Distamycin A, which binds only to B-form and not to A-form helices, binds to the triple helix without displacement of the third strand, as demonstrated by CD spectroscopy and gel electrophoresis. Molecular modeling shows that a stereochemically satisfactory structure can be build using C2'-endo sugars and a displacement of the Watson-Crick base-pair center from the helix axis of 2.5 A. Helical constraints of rise per residue (h = 3.26 A) and residues per turn (n = 12) were taken from fiber diffraction experiments of Arnott and Selsing (1974). The conformational torsion angles are in the standard B-form range, and there are no short contacts. In contrast, we were unable to construct a stereochemically allowed model with A-form geometry and C3'-endo sugars. Arnott et al. (1976) observed that their model had short contacts (e.g., 2.3 A between the phosphate-dependent oxygen on the A strand and O2 in the Hoogsteen-paired thymine strand) which are generally known to be outside the allowed range.(ABSTRACT TRUNCATED AT 250 WORDS)     

Conformational variations in d(TGACGTCA) and its reverse sequence d(ACTGCAGT): a joint circular dichroism and nuclear magnetic resonance study

Circular dichroism (CD) and nuclear magnetic resonance (NMR) techniques have been used to characterize the structural properties of the two self-complementary DNA octamers d(TGACGTCA) (I) and d(ACTGCAGT) (II). These display as distinctive features reverse sequences and central steps CpG and GpC, respectively. CD experiments lead to B-form DNA spectra characterized by larger magnitude signals in the case of octamer (I). NMR COSY spectra indicate that in the two octamers all the residues are predominantly south, S, (2'-endo) sugar conformation. NMR NOESY spectra show most of the glycosidic angles confined in the range predicted for B-form DNA although important heterogeneity is noticed along the chains, more pronounced in the case of octamer (I). Both the increase of north, N, (3'-endo) sugar conformation and P (pseudorotation phase angle) deviation from its standard B-form DNA value (162 degrees) express local sequence dependent structure distortions, remarkably visible in CpG step of octamer (I) and agreeing with NOESY cross-peaks intensities. Results interpreted according to Calladine's rules indicate higher cross-chain strains in octamer (I) than in octamer (II). All together, we find evidence to support for octamer (I) in solution local structures with A-DNA properties likely dictated by the central CpG step. Such structures could be involved in the DNA recognition by proteins and anticancerous drugs.     

Hydration of [d(CGC)r(aaa)d(TTTGCG)](2)

We have studied the hydration and dynamics of RNA C2'-OH in a DNA. RNA hybrid chimeric duplex [d(CGC)r(aaa)d(TTTGCG)](2). Long-lived water molecules with correlation time tau(c) larger than 0.3 ns were found close to the RNA adenine H2 and H1' protons in the hybrid segment. A possible long-lived water molecule was also detected close to the methyl group of 7T in the RNA-DNA junction but not to the other two thymine bases (8T and 9T). This result correlates with the structural studies that only DNA residue 7T in the RNA-DNA junction adopts an O4'-endo sugar conformation (intermediate between B-form and A-form), while the other DNA residues including 3C in the DNA-RNA junction, adopt C1'-exo or C2'-endo conformations (in the B-form domain). Based on the NOE cross-peak patterns, we have found that RNA C2'-OH tends to orient toward the O3' direction, forming a possible hydrogen bond with the 3'-phosphate group. The exchange rates for RNA C2'-OH were found to be around 5-20 s(-1), compared to 26.7(+/-13.8) s(-1) reported previously for the other DNA.RNA hybrid duplex. This slow exchange rate may be due to the narrow minor groove width of [d(CGC)r(aaa)d(TTTGCG)](2), which may trap the water molecules and restrict the dynamic motion of hydroxyl protons. The distinct hydration patterns of the RNA adenine H2 and H1' protons and the DNA 7T methyl group in the hybrid segment, as well as the orientation and dynamics of the RNA C2'-OH protons, may provide a molecular basis for further understanding the structure and recognition of DNA.RNA hybrid and chimeric duplexes.     

Thermodynamic and structural properties of pentamer DNA.DNA, RNA.RNA, and DNA.RNA duplexes of identical sequence

Four pentamers with the general sequence 5'CU(T)GU(T)G/5'CACAG have been prepared by chemical synthesis in order to generate duplex structures with common sequences. The four duplexes studied include the DNA.DNA duplex (5'dCACAG/5'dCTGTG) and the RNA.RNA duplex (5'rCUGUG/5'rCACAG) as well as the two corresponding DNA.RNA heteroduplexes (5'rCUGUG/5'dCACAG and 5'CACAG/5'dCTGTG). The measured entropy, enthalpy, and free energy changes upon melting are reported for each pentamer and compared to the predicted values where possible. Results show that the two DNA.RNA heteroduplexes are destabilized (delta G degrees 25 = -4.2 +/- 0.4 kcal/mol) relative to either the DNA.DNA duplex (delta G degrees 25 = -4.8 +/- 0.5 kcal/mol) or the RNA.RNA duplex (delta G degrees 25 = -5.8 +/- 0.6 kcal/mol). Circular dichroism spectra indicate that the RNA and the two heteroduplexes adopt an A-form conformation, while the DNA conformation is B-form. Imino proton NMR spectra also show that the heteroduplex structures resemble the RNA.RNA duplex.     

CD, absorption and thermodynamic analysis of repeating dinucleotide DNA, RNA and hybrid duplexes [d/r(AC)]12.[d/r(GT/U)]12 and the influence of phosphorothioate substitution.

Circular dichroism (CD) spectra and melting temperature (Tm) data for five duplexes containing phosphorothioate linkages were compared with data for four unmodified duplexes to assess the effect of phosphorothioate modification on the structure and stability of DNA. DNA and DNA.RNA duplexes. Nine duplexes were formed by mixing oligomers 24 nt long in 0.15 M K+(phosphate buffer), pH 7.0. Unmodified DNA.DNA and RNA.RNA duplexes were used as reference B-form and A-form structures. The CD spectra of the modified hybrids S-d(AC)12.r(GU)12 and r(AC)12.S-d(GT)12 differed from each other but were essentially the same as the spectra of the respective unmodified hybrids. They were more A-form than B-form in character. CD spectra of duplexes S-d(AC)12.d(GT)12 and d(AC)12.S-d(GT)12 were similar to that of d(AC)12.d(GT)12, except for a reduced long wavelength CD band. Sulfur modifications on both strands of the DNA duplex caused a pronounced effect on its CD spectrum. The order of thermal stability was: RNA.RNA > DNA.DNA > DNA.RNA > S-DNA.DNA > S-DNA. RNA > S-DNA.S-DNA. Phosphorothioation of one strand decreased the melting temperature by 7.8+/-0.6 degrees C, regardless of whether the substitution was in a hybrid or DNA duplex. Thermodynamic parameters were obtained from a multistate analysis of the thermal melting profiles. Interestingly, the destabilizing effect of the phosphorothioate substitution appears to arise from a difference in the entropy upon forming the DNA.DNA duplexes, while the destabilizing effect in the DNA.RNA hybrids appears to come from a difference in enthalpy.     

Solution structure of an LNA hybridized to DNA: NMR study of the d(CT(L)GCT(L)T(L)CT(L)GC):d(GCAGAAGCAG) duplex containing four locked nucleotides

We have used two-dimensional (1)H NMR spectroscopy at 750 MHz to determine a high-resolution solution structure of an oligonucleotide containing restricted nucleotides with a 2'-O, 4'-C-methylene bridge (LNA) hybridized to the complementary DNA strand. The LNA:DNA duplex examined contained four thymidine LNA modifications (T(L), d(C1T(L)2G3C4T(L)5T(L)6C7T(L)8G9C10):d( G11C12A13G14A15A16G17C 18A19G20). A total relaxation matrix approach was used to obtain interproton distance bounds from NOESY cross-peak intensities. These distance bounds were used as restraints in molecular dynamics (rMD) calculations. Forty final structures were generated for the duplex from A-form and B-form DNA starting structures. The root-mean-square deviation (RMSD) of the coordinates for the 40 structures of the complex was 0.6 A. The sugar puckerings are averaged values of a dynamic interchange between N- and S-type conformation except in case of the locked nucleotides that were found to be fixed in the C3'-endo conformation. Among the other nucleotides in the modified strand, the furanose ring of C7 and G9 is predominantly in the N-type conformation whereas that of G3 is in a mixed conformation. The furanose rings of the nucleotides in the unmodified complementary strand are almost exclusively in the S-type conformation. Due to these different conformations of the sugars in the two strands, there is a structural strain between the A-type modified strand and the B-type unmodified complementary strand. This strain is relaxed by decreasing the value of rise and compensating with tip, buckle, and propeller twist. The values of twist vary along the strand but for a majority of the base pairs a value even lower than that of A-DNA is observed. The average twist over the sequence is 32+/-1 degrees. On the basis of the structure, we conclude that the high stability of LNA:DNA duplexes is caused by a local change of the phosphate backbone geometry that favors a higher degree of stacking.     

Binding of CC-1065 to poly- and oligonucleotides

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

Structure and stability of the consecutive stereoregulated chiral phosphorothioate DNA duplex

The duplex structures of the stereoregulated phosphorothioate DNAs, [R(p),R(p)]- and [S(p),S(p)]-[d(GC(ps)T(ps)ACG)] (ps, phosphorothioate; PS-DNA), with their complementary RNA have been investigated by combined use of (1)H NMR and restrained molecular dynamics calculation. Compared to those obtained for the unmodified duplex structures (PO-DNA.RNA), the NOE cross-peak intensities are virtually identical for the PS-DNA.RNA hybrid duplexes. The structural analysis on the basis of the NOE restraints reveals that all of the three DNA.RNA duplexes take a A-form conformation and that there is no significant difference in the base stacking for the DNA.RNA hybrid duplexes. On the other hand, the NOE cross-peak intensities of the protons around the central T(ps)A step of the PS-DNA.DNA duplexes are apparently different from those of PO-DNA. DNA. The chemical shifts of H8/6 and H1' at the T(ps)A step are also largely different among PS-DNA.DNAs and PO-DNA.DNA, suggesting that the DNA.DNA structure is readily changed by the introduction of the phosphorothioate groups to the central T(p)A step. The structure calculations indicate that all of these DNA.DNA duplexes are B-form although there exist some small differences in helical parameters between the [R(p),R(p)]- and [S(p),S(p)]PS-DNA.DNA duplexes. The melting temperatures (T(m)) were determined for all of the duplexes by plotting the chemical shift change of isolated peaks as a function of temperature. For the PS-DNA.RNA hybrid duplexes, the [S(p),S(p)] isomer is less stable than the [R(p),R(p)] isomer while this trend is reversed for the PS-DNA.DNA duplexes. Consequently, although the PS-DNA.RNA duplexes take the similar A-form structure, the duplex stability is different between PS-DNA.RNA duplexes. The stability of the DNA.RNA duplexes may not be governed by the A-form structure itself but by some other factors such as the hydration around the phosphorothioate backbone, although the T(m) difference of the DNA.DNA duplexes could be explained by the structural factor.     

Molecular mechanics studies on poly(purine).poly(pyrimidine) sequences in DNA: polymorphism and local variability

Energy minimization has been carried out on three poly(purine).poly(pyrimidine) sequences--d(G)10.d(C)10, d(A)10.d(T)10, and d(AG)5.d(CT)5--using the molecular mechanics program AMBER (Assisted Model Building and Energy Refinement). In order to extensively scan the conformational space available, five different helical models were studied, three of them being right-handed helices while the other two were left helical. For all three sequences the right-handed A- and B-type helices are energetically slightly preferred over the left helices, but the energy difference between the various right-handed helices is only marginal. A detailed analysis has been carried out to characterize the local structural variability in the refined structures, both in terms of torsion angles as well as other parameters such as base-pair tilt, wedge roll, and wedge tilt, etc. All three sequences exhibit similar structural features for a particular form, but both the forms A and B show significant deviations from fiber models. In particular, the A-form structures have higher unit rise (2.7 A), and lower unit twist (31 degrees) and base-pair tilt (12 degrees), compared to the fiber model, which has corresponding values of 2.56 A, 32.7 degrees, and 20 degrees, respectively. All these changes indicate that the refined models are closer to the A-form structure observed in crystals of oligonucleotides. In the refined B-for models, the helical parameters are close to the fiber B-form, although the torsion angles show considerable variations. None of the three sequences examined, including the d(A)n.d(T)n sequence, show any pronounced curvature for the B-form structure.     

A duplex of the oligonucleotides d(GGGGGTTTTT) and d(AAAAACCCCC) forms an A to B conformational junction in concentrated salt solutions

The coexistence of both A form and B form tracts and formation of an A-B junction in the oligomer d(GGGGGTTTTT).d(AAAAACCCCC) in saturated sodium chloride solution have been detected by Raman spectroscopy. The entire duplex adopts the familiar B-form conformation in aqueous solution at low salt concentrations (0.1M NaCl). In 6M NaCl the adoption of an A form is observed within the G,C tract while a B-form is maintained in the A.T tract. The experimental results indicate that two different helical forms can co-exist in a rather short oligonucleotide and that formation of an A-B junction can occur over a fairly small span of bases. This is in agreement with recent rules governing the relation between base sequence and secondary structure of DNA published from this laboratory. The conformational preferences of each of the individual oligomers d(AAAAACCCCC) and d(GGGGGTTTTT) have also been investigated. The oligomer d(AAAAACCCCC) is single stranded but some evidence for base stacking is observed at 2 degrees C. In contrast, a double stranded B-form structure characterized by wobble G-T base pairing is observed for d(GGGGGTTTTT) in 0.1M and 6M NaCl.     

UV-induced interstrand cross-linking of d(GT)n.d(CA)n is facilitated by a structural transition

Photochemical alterations following ultraviolet irradiation of the alternating copolymer d(GT)n.d(CA)n were studied. We found that in solution conditions which produced circular dichroism spectra compatible with B-form or A-form DNA, no interstrand cross-linking or photoproduct formation could be demonstrated. Zimmer et al. (Zimmer, C., Tymen, S., Marck, C., and Guschlbaumer, W. (1982) Nucleic Acids Res. 10, 1081-1091) and Vorlickova et al. (Vorlickova, M., Kypr, J., Sotkrova, S., Sponar, J. (1982) Nucleic Acids Res. 10, 1071-1080) have reported a number of solution conditions which produce a structural transition of this polymer characterized by a negative deviation of the circular dichroism spectrum in the region of 280 nm. The nature of this transition has not yet been elucidated. Following ultraviolet irradiation of d(GT)n.d(CA)n under two conditions which produce this transition (manganese solution or ethanol plus trace salts solution) we found ultraviolet dose-dependent interstrand cross-linking as well as dose-dependent formation of thymine-containing photoproduct. Interstrand cross-linking is demonstrated by two criteria: increase in polymer size as detected by alkaline agarose gel electrophoresis, and generation of intermediate density material in alkaline cesium sulfate isopycnic gradients. The thymine-containing photo-product was demonstrated by thin layer chromatography of acid hydrolysates of the polymer. The photo-product is at least partially photoreversible. These findings suggest that the geometry of the alternative conformation is such that pyrimidines from different strands are closely approximated, allowing for photodimerization.     

B--Z conformational transition in d(CGCGCGTTAATT), d(CGCGCGTTAA) and d(CGCGCGTT)

Conformational studies on three DNA-oligomers (d(CGCGCGTTAATT), d(CGCGTTAA) and d(CGCGCGTT) in solution by circular dichroism spectroscopy are reported. In low salt solution, all three DNA oligomers exhibit a characteristic B-conformation. However, under the influence of high salt concentration i.e. 5M NaCl, the octamer d(CGCGCGTT) exhibits 'A' conformation whereas the decamer and dodecamer retain B-conformation. On addition of millimolar amount of NiCl2 to the 5M NaCl, solution of oligodeoxynucleotides a B-Z transition is observed in octamer, decamer and dodecamer. However, NiCl2 titrations show that mid point of transition for dodecamer is at 2.25 mM, for decamer is at 13 mM NiCl2 and for octamer is 17 mM at NiCl2. In 60% alcohol all three oligonucleotides remain in the B-conformation. The melting temperatures of oligonucleotides at various salt concentration are also reported. Thermodynamic parameters calculated by melting profile using a two state model show that dodecamer and decamer are most stable in their 5M NaCl, B-form. However, octamer is more stable in its Z form than that of its 'A' form.     

NMR studies of a deoxyribodecanucleotide containing an extrahelical thymidine surrounded by an oligo(dA).oligo(dT) tract

One- and two-dimensional NMR experiments were carried out on a decamer, d-(CGCTTTTCGC).d(GCGAAAAGCG), and on the same sequence with the addition of an unpaired thymidine, d(CGCTTTTCGC).d(GCGAATAAGCG), which will be referred to as the T-bulge decamer. Evidence from one-dimensional NOE experiments on the exchangeable protons indicates that the unpaired thymidine is extrahelical. This conclusion is also supported by numerous cross-peaks in the two-dimensional NOESY spectrum of the nonexchangeable protons. Assignments for all of the resonances, with the exception of the H5' and H5" resonances, have been made for both oligonucleotide duplexes through the use of 2D NOESY, COSY, and relayed COSY experiments. Temperature dependence of the methyl resonance chemical shifts indicates that the unpaired thymidine shows unusual behavior compared to other thymidines in the duplex. Two-dimensional NOESY experiments carried out from 5 to 35 degrees C indicate the unpaired thymidine remains extrahelical throughout this temperature range. A similar temperature dependence for the methyl chemical shift is found in the corresponding single-strand d(GCGAATAAGCG). The oligo-(dA).oligo(dT) tracts in both the decamer and the T-bulge decamer have structures different from B-form DNA and exhibit NOEs similar to those observed in other oligonucleotides containing A.T tracts. The formation of this unusual A.T tract structure may induce the extrahelical conformation of the unpaired thymidine.     

A Duplex of the Oligonucleotides d(GGGGGTTTTT) and d(AAAAACCCCC) Forms an A to B Conformational Junction in Concentrated Salt Solutions

Abstract

The coexistence of both A form and B form tracts and formation of an A-B junction in the oligomer d(GGGGGTTTTT)· d(AAAAACCCCC) in saturated sodium chloride solution have been detected by Raman spectroscopy. The entire duplex adopts the familiar B-form conformation in aqueous solution at low salt concentrations (0.1M NaCl). In 6M NaCl the adoption of an A form is observed within the G,C tract while a B-form is maintained in the A,T tract. The experimental results indicate that two different helical forms can co-exist in a rather short oligonucleotide and that formation of an A-B junction can occur over a fairly small span of bases. This is in agreement with recent rules governing the relation between base sequence and secondary structure of DNA published from this laboratory.

The conformational preferences of each of the individual oligomers d(AAAAACCCCC) and d(GGGGGTTTTT) have also been investigated. The oligomer d(AAAAACCCCC) is single stranded but some evidence for base stacking is observed at 2°C. In contrast, a double stranded B-form structure characterized by wobble G-T base pairing is observed for d(GGGGGTTTTT) in 0.1M and 6M NaCl.