Parallel-stranded DNA with natural base sequences

Noncanonical parallel-stranded DNA double helices (ps-DNA) comprising natural nucleotide sequences are usually second in stability to antiparallel-stranded (aps) canonical DNA structures, which ensures reliable cell functioning. However, recent data indicate a possible role of ps-DNA in DNA loops or in trinucleotide repeats connected with neurodegenerative diseases. The review surveys recent studies on the effect of nucleotide sequence on preference of one or other type of DNA duplex. (1) Ps-DNA with mixed AT/GC composition was found to have conformational and thermodynamic properties drastically different from those of Watson-Crick double helix. Its stability depends strongly on the specific sequence in a manner peculiar to the ps double helix, because of the energy disadvantage of the AT/GC contacts. The AT/GC boundary facilitated flipping of A and T out of the ps double helix. Proton acceptor groups of bases are exposed into the both grooves of the ps-DNA and are accessible to solvent and ligands, including proteins. (2) DNA regions containing natural minor bases isoguanine and isomethylcytosine were shown to form ps-DNA with transAT-, trans isoGC, and trans iso5meCG pairs exceeding in stability a related aps duplex. (3) Nucleotide sequence dG(GT)4G from yeast telomeres and microsatellites was demonstrated to form novel ps-DNA with GG and TT base pairing. Unlike d(GT)n and d(GnTm) sequences able to form quadruplexes, the dG(GT)4G sequence formed no alternative double- or multistranded structures in a wide range of experimental conditions, thus suggesting that the nucleotide context governs the observed structural polymorphism of the d(GT)n sequence. The possible biological role of ps-DNA and the prospects of its study are discussed.     

Parallel-Stranded DNA with Natural Base Sequences

Noncanonical parallel-stranded DNA double helices (ps-DNA) of natural nucleotide sequences are usually less stable than the canonical antiparallel-stranded DNA structures, which ensures reliable cell functioning. However, recent data indicate a possible role of ps-DNA in DNA loops or in regions of trinucleotide repeats connected with neurodegenerative diseases. The review surveys recent studies on the effect of nucleotide sequence on preference of one or other type of DNA duplex. (1) Ps-DNA of mixed AT/GC composition was found to have conformational and thermodynamic properties drastically different from those of a Watson–Crick double helix. Its stability depends strongly on the specific sequence in a manner peculiar to the ps double helix, because of the energy disadvantage of the AT/GC contacts. The AT/GC boundary facilitated flipping of A and T out of the ps double helix. Proton acceptor groups of bases are exposed into both grooves of the ps-DNA and are accessible to solvent and ligands, including proteins. (2) DNA regions containing natural minor bases isoguanine and isomethylisocytosine were shown to form ps-DNA with transAT-, trans isoGC, and transiso^5meCG pairs exceeding in stability a related canonical duplex. (3) Nucleotide sequence dG(GT)₄G from yeast telomeres and microsatellites was demonstrated to form novel ps-DNA with GG and TT base pairing. Unlike d(GT) _n - and d(G _n T _m ) sequences able to form quadruplexes, the dG(GT)₄G sequence formed no alternative double- or multistranded structures in a wide range of experimental conditions, thus suggesting that the nucleotide context governs the observed structural polymorphism of the d(GT) _n sequence. The possible biological role of ps-DNA and the prospects of its study are discussed.     

Parallel-stranded duplex DNA containing blocks of trans purine-purine and purine-pyrimidine base pairs.

A 30 base pair parallel-stranded (ps) duplex ps-L1.L2 composed of two adjoined purine-purine and purine-pyrimidine sequence blocks has been characterized thermodynamically and spectroscopically. The 5'-terminal 15 residues in both strands ('left-half') consisted of the alternating d(GA)7G sequence that forms a ps homoduplex secondary structure stabilized by d(G.G) and d(A.A) base pairs. The 3'-terminal 15 positions of the sequence ('right-half') were combinations of A and T with complementary reverse Watson-Crick d(A.T) base pairing between the two strands. The characteristics of the full length duplex were compared to those of the constituent left and right halves in order to determine the compatibility of the two ps helical forms. The thermal denaturation curves and hyperchromicity profiles of all three duplexes determined by UV absorption spectroscopy were characteristic of ps-DNA, in accordance with previous studies. The thermodynamic properties of the 30 bp duplex corresponded within experimental error to the linear combination of the two 15-mers. Thus, the Tm and delta HvH of ps-L1.L2 in 10 mM MgCl2, derived from analyses according to a statistical mechanical formulation for the helix-coil transition, were 43 degrees C and 569 kJ mol-1, compared to 21 degrees C, 315 kJ mol-1 (ps-F5.F6) and 22 degrees C, 236 kJ mol-1 (ps-GA15). The UV absorption and CD spectra of ps-L1.L2 and the individual 15-mer ps motifs were also compared quantitatively. The sums of the two constituent native spectra (left+right halves) accurately matched that of the 30 bp duplex, with only small deviations in the 195-215 nm (CD) and 220-240 nm (absorption) regions. Based on analysis by native gel electrophoresis, the sequences studied formed duplex structures exclusively; there were no indications of higher order species. Chemical modification with diethyl pyrocarbonate showed no hyperreactivity of the junctional bases, indicating a smooth transition between the two parallel-stranded conformations. We conclude that under given salt conditions, oligonucleotides with normal primary chemical structures can readily form a parallel-stranded double helix based on blocks of very disparate non-canonical purine-purine and purine-pyrimidine base pairs and without perceptible destabilization at the junction. There are biological implications of these findings in relation to genetic structure and expression.     

The stability of duplexes involving AT and/or G4EtC base pairs is not dependent on their AT/G4EtC ratio content. Implication for DNA sequencing by hybridization.

Sequencing by the recently reported hybridization technique requires the formation of DNA duplexes with similar stabilities. In this paper we describe a new strategy to obtain DNA duplexes with a thermal stability independent of their AT/GC ratio content. Melting data were acquired on 35 natural and 27 modified duplexes of a given length and of varying base compositions. Duplexes built with AT and/or G4EtC base pairs exhibit a thermal stability restrained to a lower range of temperature than that of the corresponding natural compounds (16 instead of 51 degrees C). The 16 degrees C difference in thermal stability observed between the least stable and the most stable duplex built with AT and/or G4EtC base pairs is mainly due to the sequence effect and not to their AT/G4EtC ratio content. Thus N -4-ethyl-2'-deoxycytidine (d4EtC) hybridizes specifically with natural deoxyguanosine leading to a G4EtC base pair whose stability is very close to that of the natural AT base pair. Oligonucleotide probes involving d4EtC can be easily prepared by chemical synthesis with phosphoramidite chemistry. Modified DNA targets were successfully amplified by random priming or PCR techniques using d4EtCTP, dATP, dGTP and dTTP in the presence of DNA polymerase. This new system might be very useful for DNA sequencing by hybridization.     

Isolation and characterization of thermodynamically stable and unstable RNA hairpins from a triloop combinatorial library

Hairpins are the most common elements of RNA secondary structure, playing important roles in RNA tertiary architecture and forming protein binding sites.Triloops are common in a variety of naturally occurring RNA hairpins, but little is known about their thermodynamic stability. Reported here are the sequences and thermodynamic parameters for a variety of stable and unstable triloop hairpins. Temperature gradient gel electrophoresis (TGGE) can be used to separate a simple RNA combinatorial library based on thermal stability [Bevilacqua, J. M., and Bevilacqua, P. C. (1998) Biochemistry 45, 15877-15884]. Here we introduce the application of TGGE to separating and analyzing a complex RNA combinatorial library based on thermal stability, using an RNA triloop library. Several rounds of in vitro selection of an RNA triloop library were carried out using TGGE, and preferences for exceptionally stable and unstable closing base pairs and loop sequences were identified. For stable hairpins, the most common closing base pair is CG, and U-rich loop sequences are preferred. Closing base pairs of GC and UA result in moderately stable hairpins when combined with a stable loop sequence. For unstable hairpins, the most common closing base pairs are AU and UG, and U-rich loop sequences are no longer preferred. In general, the contributions of the closing base pair and loop sequence to overall hairpin stability appear to be additive. Thermodynamic parameters for individual hairpins determined by UV melting are generally consistent with outcomes from selection experiments, with hairpins containing a CG closing base pair having a DeltaDeltaG degrees (37) 2.1-2.5 kcal/mol more favorable than hairpins with other closing base pairs. Sequences and thermodynamic rules for triloop hairpins should aid in RNA structure prediction and determination of whether naturally occurring triloop hairpins are thermodynamically stable.     

Effects of flanking G . C base pairs on internal Watson-Crick, G . U, and nonbonded base pairs within a short ribonucleic acid duplex

A series of pentaribonucleotides, ApGpXpGpU (where X identical to A, G, C, or U), was synthesized to investigate the effects of flanking G . C pairs on internal Watson-Crick, G . U, and nonbonded base pairs. Sequences ApGpApCpU (Tm = 26 degrees C) and ApGpCpCpU (Tm = 25 degrees C) were each found to form a duplex with non-base-paired internal residues that stacked with the rest of the sequence but were not looped out. ApGpGpCpU also forms a duplex (Tm = 30 degrees C) but with dangling terminal nonbonded adenosines rather than internal nonbonded guanosines. ApGpUpCpU prefers a stacked single-strand conformation. In addition, contribution to duplex stability from an internal A . U or G . C base pair is enhanced by 6 degrees C when flanked by G . C base pairs as compared to A . U base pairs. G . C base pairs flanking an internal G . U base pair were found to be more tolerant to the altered conformation of a G . U pair and result in an increase to stability comparable with that found for an internal A . U base pair.     

Thermodynamic parameters for loop formation in RNA and DNA hairpin tetraloops.

We determined the melting temperatures (Tm) and thermodynamic parameters of 15 RNA and 19 DNA hairpins at 1 M NaCl, 0.01 M sodium phosphate, 0.1 mM EDTA, at pH 7. All these hairpins have loops of four bases, the most common loop size in 16S and 23S ribosomal RNAs. The RNA hairpins varied in loop sequence, loop-closing base pair (A.U, C.G, or G.C), base sequence of the stem, and stem size (four or five base pairs). The DNA hairpins varied in loop sequence, loop-closing base pair (C.G, or G.C), and base sequence of the four base-pair stem. Thermodynamic properties of a hairpin may be represented by nearest-neighbor interactions of the stem plus contributions from the loop. Thus, we obtained thermodynamic parameters for the formation of RNA and DNA tetraloops. For the tetraloops we studied, a free energy of loop formation (at 37 degrees C) of about +3 kcal/mol is most common for either RNA or DNA. There are extra stable loops with delta G degrees 37 near +1 kcal/mol, but the sequences are not necessarily the same for RNA and DNA. The closing base pair is also important; changing from C.G to G.C lowered the stability of several tetraloops in both RNA and DNA. These values will be useful in predicting RNA and DNA secondary structures.     

A parallel stranded linear DNA duplex incorporating dG.dC base pairs

DNA oligonucleotides with appropriately designed complementary sequences can form a duplex in which the two strands are paired in a parallel orientation and not in the conventional antiparallel double helix of B-DNA. All parallel stranded (ps) molecules reported to date have consisted exclusively of dA.dT base pairs. We have substituted four dA.dT base pairs of a 25-nt parallel stranded linear duplex (ps-D1.D2) with dG.dC base pairs. The two strands still adopt a duplex structure with the characteristic spectroscopic properties of the ps conformation but with a reduced thermodynamic stability. Thus, the melting temperature of the ps duplex with four dG.dC base pairs (ps-D5.D6) is 10-16 degrees C lower and the van't Hoff enthalpy difference delta HvH for the helix-coil transition is reduced by 20% (in NaCl) and 10% (in MgCl2) compared to that of ps-D1.D2. Based on energy minimizations of a ps-[d(T5GA5).d(A5CT5)] duplex using force field calculations we propose a model for the conformation of a trans dG.dC base pair in a ps helix.     

Structure and drug interactions of parallel-stranded DNA studied by infrared spectroscopy and fluorescence.

The infrared spectra of three different 25-mer parallel-stranded DNAs (ps-DNA) have been studied. We have used ps-DNAs containing either exclusively dA x dT base pairs or substitution with four dG x dC base pairs and have them compared with their antiparallel-stranded (aps) reference duplexes in a conventional B-DNA conformation. Significant differences have been found in the region of the thymine C = O stretching vibrations. The parallel-stranded duplexes showed characteristic marker bands for the C2 = O2 and C4 = O4 carbonyl stretching vibrations of thymine at 1685 cm-1 and 1668 cm-1, respectively, as compared to values of 1696 cm-1 and 1663 cm-1 for the antiparallel-stranded reference duplexes. The results confirm previous studies indicating that the secondary structure in parallel-stranded DNA is established by reversed Watson--Crick base pairing of dA x dT with hydrogen bonds between N6H...O2 and N1...HN3. The duplex structure of the ps-DNA is much more sensitive to dehydration than that of the aps-DNA. Interaction with three drugs known to bind in the minor groove of aps-DNA--netropsin, distamycin A and Hoechst 33258--induces shifts of the C = O stretching vibrations of ps-DNA even at low ratio of drug per DNA base pair. These results suggest a conformational change of the ps-DNA to optimize the DNA-drug interaction. As demonstrated by excimer fluorescence of strands labeled with pyrene at the 5'-end, the drugs induce dissociation of the ps-DNA duplex with subsequent formation of imperfectly matched aps-DNA to allow the more favorable drug binding to aps-DNA. Similarly, attempts to form a triple helix of the type d(T)n.d(A)n.d(T)n with ps-DNA failed and resulted in the dissociation of the ps-DNA duplex and reformation of a triple helix based upon an aps-DNA duplex core d(T)10.d(A)10.     

Characterization of ciprofloxacin binding to the linear single- and double-stranded DNA

The binding of ciprofloxacin to natural and synthetic polymeric DNAs was investigated at different solvent conditions using a combination of spectroscopic and hydrodynamic techniques. In 10 mM cacodylate buffer (pH 7.0) containing 108.6 mM Na(+), no sequence preferences in the interaction of ciprofloxacin with DNA was detected, while in 2 mM cacodylate buffer (pH 7.0) containing only 1.7 mM Na(+), a significant binding of ciprofloxacin to natural and synthetic linear double-stranded DNA was observed. At low ionic strength of solution, ciprofloxacin binding to DNA duplex containing alternating AT base pairs is accompanied by the largest enhancement in thermal stability (e.g. DeltaT(m) approximately 10 degrees C for poly[d(AT)].poly[d(AT)]), and the most pronounced red shift in the position of the maximum of the fluorescence emission spectrum (lambda(max)). Similar red shift in the position of lambda(max) is also observed for ciprofloxacin binding to dodecameric duplex containing five successive alternating AT base pairs in the row. On the other hand, ciprofloxacin binding to poly[d(GC)].poly[d(GC)], calf thymus DNA and dodecameric duplex containing a mixed sequence is accompanied by the largest fluorescence intensity quenching. Addition of NaCl does not completely displace ciprofloxacin bound to DNA, indicating the binding is not entirely electrostatic in origin. The intrinsic viscosity data suggest some degree of ciprofloxacin intercalation into duplex.     

Helix-coil transition of parallel-stranded DNA. Thermodynamics of hairpin and linear duplex oligonucleotides

The stabilities have been determined of different DNA double helices constructed with the two constituent strands in a parallel orientation. These molecules incorporate polarity-inverting loop structures (hairpins) or nucleotide sequences (duplexes) which impose the desired polarity on the two strands constituting the sugar-phosphate backbone. The hairpins consisted of d(A.T)n stems (n = 8 or 10) and either a 5'-p-5' linkage in a d(C)4 loop (ps-C8 and ps-C10) or a 3'-p-3' linkage in a d(G)4 loop (ps-G10). The linear duplexes had 21-nt (ps-C2.C3) and 25-nt (ps-D1.D2, ps-D3.D4) mixed A,T sequences and normal chemical linkages throughout. Reference molecules with normal antiparallel helical orientations (hairpins aps-C8, aps-C10, and aps-G10 and duplexes aps-C3.C7, aps-D1.D3, and aps-D2.D4) were also synthesized and studied. Hydrogen bonding in ps-DNA is via reverse Watson-Crick base pairs, and the various constructs display spectroscopic, chemical, biochemical, and electrophoretic properties distinct from those of their aps counterparts. For example, both the ps and aps molecules show a pronounced UV absorption hyperchromicity upon melting, but the spectral distribution is not the same. Thus, the difference spectra (ps-aps) in the native state are characterized by a positive peak at 252 nm, an isosbestic point at 267 nm, and a negative peak at 282 nm. Temperature-dependent absorbances were recorded at selected wavelengths and in the form of complete spectra to derive the thermodynamic parameters for the helix-coil transitions.(ABSTRACT TRUNCATED AT 250 WORDS)     

Parallel-stranded duplex DNA containing dA · dU base pairs

DNA oligonucleotides with dA and dU residues can form duplexes with trans d(A · U) base pairing and the sugar-phosphate backbone in a parallel-stranded orientation, as previously established for oligonucleotides with d(A · T) base pairs. The properties of such parallel-stranded DNA (ps-DNA) 25-mer duplexes have been characterized by absorption (uv), CD, ir, and fluorescence spectroscopy, as well as by nuclease sensitivity. Comparisons were made with duplex molecules containing (a) dT in both strands, (b) dU in one strand and dT in the second, and (c) the same base combinations in reference antiparallel-stranded (aps) structures. Thermodynamic analysis revealed that total replacement of deoxythymine by deoxyuridine was accompanied by destabilization of the ps-helix (reduction in T_m by −13°C in 2 mM MgGl₂, 10 mM Na-cacodylate). The U-containing ps-helix (U1 · U2) also melted 14°C lower than the corresponding aps-helix under the same ionic conditions; this difference was very close to that observed between ps and aps duplexes with d(A · T) base pairs. Force field minimized structures of the various ps and aps duplexes with either d(A · T) or d(A · U) base pairs ps/aps and dT/dU combinations are presented. The energy-minimized helical parameters did not differ significantly between the DNAs containing dT and dU. © 1996 John Wiley & Sons, Inc.     

High resolution NMR study of CAP binding site 22mer in H2O solution

High resolution proton NMR were measured for the deoxyoligonucleotide 22mer duplex corresponding to the CAP (catabolite gene activator protein) binding site of lac promotor. The spectra in the lower field region than the water resonance were taken with the time-shared Redfield pulse method by using a JEOL 500 MHz NMR spectrometer. In the imino proton region 18 peaks were separately observed, but the area intensity at 10 degrees C corresponds to 20 protons. By selective irradiation at each peak position NOEs (nuclear Overhauser effects) were observed between the imino and adenine C2H protons and between imino proton themselves. By tracing sequential NOE train carefully, 17 imino proton signals could be unambiguously assigned to each base pair except five AT base pairs at terminals. With the elevation of temperature the peaks showed gradual broadening and disappeared, which indicates the stepwise base pair opening of the duplex. Referring to the above peak assignments it can be concluded that GC20 and AT4 pairs close to terminals relax first and the base pair opening proceeds toward central GC13 and 14.     

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.     

Enhanced base-pair opening in the adenine tract of a RNA double helix

Proton exchange and nuclear magnetic resonance spectroscopy are being used to characterize the kinetics and energetics of base-pair opening in two nucleic acid double helices. One is the RNA duplex 5'-r(GCGAUAAAAAGGCC)-3'/5'-r(GGCCUUUUUAUCGC)-3', which contains a central tract of five AU base pairs. The other is the homologous DNA duplex with a central tract of five AT base pairs. The rates and the equilibrium constants of the opening reaction of each base pair are measured from the dependence of the exchange rates of imino protons on ammonia concentration, at 10 °C. The results reveal that the tract of AU base pairs in the RNA duplex differs from the homologous tract of AT base pairs in DNA in several ways. The rates of opening of AU base pairs in RNA are high and increase progressively along the tract, reaching their largest values at the 3'-end of the tract. In contrast, the opening rates of AT base pairs in DNA are much lower than those of AU base pairs. Within the tract, the largest opening rate is observed for the AT base pair at the 5'-end of the tract. These differences in opening kinetics are paralleled by differences in the stabilities of individual base pairs. All AU base pairs in the RNA are less stable than the AT base pairs in the DNA. The presence of the tract enhances these differences by increasing the stability of AT base pairs in DNA while decreasing the stability of AU base pairs in RNA. Due to these divergent trends, along the tracts, the AU base pairs become progressively less stable than AT base pairs. These findings demonstrate that tracts of AU base pairs in RNA have specific dynamic and energetic signatures that distinguish them from similar tracts of AT base pairs in DNA.     

Free energy contributions of G.U and other terminal mismatches to helix stability

Thermodynamic parameters of helix formation were measured spectroscopically for seven hexaribonucleotides containing a GC tetramer core and G.U or other terminal mismatches. The free energies of helix formation are compared with those for the tetramer core alone and with those for the hexamer with six Watson-Crick base pairs. In 1 M NaCl, at 37 degrees C, the free energy of a terminal G.U mismatch is about equal to that of the corresponding A.U pair. Although other terminal mismatches studied add between -1.0 and -1.6 kcal/mol to delta G0 37 for helix formation, all are less stable than the corresponding Watson-Crick pairs. Comparisons of the stability increments for terminal G.U mismatches and G.C pairs suggest when stacking is weak the additional hydrogen bond in the G.C pair adds roughly -1 kcal/mol to the favorable free energy of duplex formation.     

1H NMR determination of base-pair lifetimes in oligonucleotides containing single base mismatches

Proton nuclear magnetic resonance (NMR) spectroscopy is employed to characterize the kinetics of base-pair opening in a series of 9mer duplexes containing different single base mismatches. The imino protons from the different mismatched, as well as fully matched, duplexes are assigned from the imino-imino region in the WATERGATE NOESY spectra. The exchange kinetics of the imino protons are measured from selective longitudinal relaxation times. In the limit of infinite exchange catalyst concentration, the exchange times of the mismatch imino protons extrapolate to much shorter lifetimes than are commonly observed for an isolated GC base pair. Different mismatches exhibit different orders of base-pair lifetimes, e.g. a TT mismatch has a shorter base-pair lifetime than a GG mismatch. The effect of the mismatch was observed up to a distance of two neighboring base pairs. This indicates that disruption in the duplex caused by the mismatch is quite localized. The overall order of base-pair lifetimes in the selected sequence context of the base pair is GC > GG > AA > CC > AT > TT. Interestingly, the fully matched AT base pair has a shorter base-pair lifetime relative to many of the mismatches. Thus, in any given base pair, the exchange lifetime can exhibit a strong dependence on sequence context. These findings may be relevant to the way mismatch recognition is accomplished by proteins and small molecules.     

Distamycin-stabilized Antiparallel-Parallel Combination (APC) DNA

Abstract

The formation of Antiparallel-Parallel-Combination (APC) DNA, a liner duplex with a segment of parallel-stranded (ps) helix flanked by conventional B-DNA, was tested with a number of synthetic oligonucleotides. The groove-binding ligand distamycin A (DstA) was used to stabilize the ps segment comprising five A·T base pairs. Two drug molecules bound per APC, one in each of the two equivalent grooves characteristic of ps-DNA. APC-DNA, reference molecules and their complexes with DstA were analysed by several methods: circular dichroism and absorption spectroscopy, thermal denaturation, chemical modification, and molecular modeling. The dye binding stoichiometry differed significantly due to inherent structural differences in the groove geometries of ps-DNA (trans base pairs, similar grooves) and conventional antiparallel-stranded (aps) B-DNA (cis base pairs, distinct major and minor grooves). The data support the existence of APC folding in solution.     

Nuclear magnetic resonance structural studies of intramolecular purine.purine.pyrimidine DNA triplexes in solution. Base triple pairing alignments and strand direction

Recently, P.A. Beal and P.B. Dervan, expanding on earlier observations by others, have established the formation of purine.purine.pyrimidine triple helices stabilized by G.GC, A.AT and T.AT base triples where the purine-rich third strand was positioned in the major groove of the Watson-Crick duplex and anti-parallel to its purine strand. The present nuclear magnetic resonance (n.m.r.) study characterizes the base triple pairing alignments and strand direction in a 31-mer deoxyoligonucleotide that intramolecularly folds to generate a 7-mer (R/Y-)n.(R+)n(Y-)n triplex with the strands linked by two T5 loops and stabilized by potential T.AT and G.GC base triples. (R and Y stand for purine and pyrimidine, respectively, while the signs establish the strand direction.) This intramolecular triplex gives well-resolved exchangeable and non-exchangeable proton spectra with Li+ as counterion in aqueous solution. These studies establish that the T1 to C7 pyrimidine and the G8 to A14 purine strands are anti-parallel to each other and align through Watson-Crick A.T and G.C pair formation. The T15 to G21 purine-rich third strand is positioned in the major groove of this duplex and pairs through Hoogsteen alignment with the purine strand to generate T.AT and G.GC triples. Several lines of evidence establish that the thymidine and guanosine bases in the T15 to G21 purine-rich third strand adopt anti glycosidic torsion angles under conditions where this strand is aligned anti-parallel to the G8 to A14 purine strand. We have also recorded imino proton n.m.r. spectra for an (R-)n.(R+)n(Y-)n triplex stabilized by G.GC and A.AT triples through intramolecular folding of a related 31-mer deoxyoligonucleotide with Li+ as counterion. The intramolecular purine.purine.pyrimidine triplexes containing unprotonated G.GC, A.AT and T.AT triples are stable at basic pH in contrast to pyrimidine.purine.pyrimidine triplexes containing protonated C+.GC and T.AT triples, which are only stable at acidic pH.