Spectroscopic studies on the structure of poly(8-bromoadenylic acid): Effect of glycosidic torsion angle on the conformation and flexibility in polyribonucleotides

The helix–coil transition and conformational structure of poly(8-bromoadenylic acid) [poly(8BrA)] have been investigated using ¹H- and ¹³C-nmr, CD, and ir spectroscopy. The results have been compared with the structure of the related 5′-mono- and polynucleotides. The chemical shifts of H(2′), H(3′), C(2′), and C(3′) nmr signals show an interesting correlation with both the puckering of ribose ring and glycosidic bond torsion angle. Poly(8BrA) shows an upfield shift of the C(3′) signal and a downfield shift of the H(3′) signal compared to the chemical shifts in poly(A). These shifts are consistent with a C(3′) endo-syn conformation for poly(8BrA). A similar effect has been reported previously and is also observed here on the C(2′) and H(2′) signals when the preferred conformation is C(2′)endo-syn (e.g., in 5′-8BrAMP). The chemical-shift parameters thus act as a probe for studying syn ? anti and N ? S equilibria in solutions. The three-bond ¹H-′¹³C coupling constants between H(1′) and C(8) and C(4) have been measured in poly(8BrA) and 5′-8BrAMP and their structural implications have been discussed. The observed preference of a C(3′)endo-syn conformation for poly(8BrA), coupled with other evidence, throws doubt on the validity of a correlation previously reported whereby a syn conformation is associated with a C(2′)endo ribose pucker. The backbone conformation of randomly coiled poly(8BrA) is very similar to the structures found in polyribonucleotides: poly(A) and poly(U). All three polymers show strong preferences for the backbone angles found in RNA helices. The CD spectrum of poly(8BrA) has a striking relationship to that of poly(A). The signs of all extrema are inverted, and the magnitudes are related by a constant factor. We suggest that these differences result from a change in the angle between coupled transition moment vectors in the two polymers. Infrared spectra of poly(8BrA) in H₂O and D₂O solution are reported for the frequency range below 1400 cm^?1. The antisymmetric >PO stretching vibration is observed at an unusually low frequency in the helix (1214 cm^?1). The symmetric >PO stretch occurs at ～1095 cm^?1 but is not resolved from a ring vibration near this frequency. A conformationally sensitive band, characteristic of helical RNA structures, is observed at 817 cm^?1 and disappears when the helix is melted. This observation confirms the conclusion that ordered poly(8BrA) has a regular helical structure with an RNA backbone conformation. A stereochemical explanation is provided for the failure of poly(8BrA) (or other syn polymers) to form double helices with anti-polyribonucleotides.     

Physical studies of the interaction of a calf thymus helix-destablizing protein with nucleic acids

UP1, a calf thymus protein that destabilizes both DNA and RNA helices, dramatically accelerates the conversion of the inactive conformers of several small RNA molecules to their biologically active forms [Karpel, R. L., Swistel, D. G., Miller, N. S., Geroch, M. E., Lu, C., & Fresco, J. R. (1974) Brookhaven Symp. Biol. 26, 165-174]. Using circular dichroic and spectrophotometric methods, we have studied the interaction of this protein with a variety of synthetic polynucleotides and yeast tRNA3Leu. As judged by perturbations in polynucleotide ellipticity or ultraviolet absorbance, the secondary structures of the single-stranded helices poly(A) and poly(C), as well as the double-stranded helices poly[d(A-T)] and poly(U.U), are largely destroyed upon interaction with UP1 at low ionic strength. This effect can be reversed by an increase in [Na+]: half the UP1-induced perturbation of the poly(A) CD spectrum is removed at 0.05 M Na+. The variation of poly(A) ellipticity and ultraviolet absorbance with [UP1]/[poly(A)]p is used to determine the length of single-stranded polynucleotide chain covered by the protein: 7 +/- 1 residues. A model is presented in which the specificity of UP1 for single strands and their concomitant distortion are a consequence of maximal binding of nucleic acid phosphates to a unique matrix of basic residues on the protein. Analogous to the effect on polynucleotides, UP1-facilitated renaturation of yeast tRNA3Leu follows the partial destruction of the inactive tRNA's secondary structure. At the tRNA absorbance maximum, UP1 effects a hyperchromic change of 10%, representing one-third of the secondary structure of the inactive conformer. This change is also clearly observable as a perturbation of the tRNA's circular dichroism spectrum.     

Study of conformation characteristics of "X-form" of alternating polynucleotides by the method of slow 1H----3H transition

The rate constants of 1H----3H exchange between water and C8H-groups of purine residues of alternating polynucleotides: poly[d(A-C)].poly[d(G-T)] and poly[d(A-T)].poly[d(A-T)], as well as Escherichia coli DNA, dAMP and dGMP, in solutions with high concentration (4.3 or 6 M) CsF, in water ethanol (60%) solution and (in comparison) in 0.15 M NaCl were determined at 25 degrees C. The 1H----3H exchange rate exchange rate constants for adenylic (kA) and guanylic (kG) residues of polynucleotides were compared with the corresponding constant for DNA and mononucleotides. It was shown that at conditions when poly[d(G-T)] and poly[d(A-T)].poly[d(A-T)] exhibit the "X-form" CD spectrum, alteration of exchange rates in polynucleotides (approximately 2-fold increase in kA in CSF and approximately 1.5-fold decrease in kA and kG in 60% ethanol with 0.15 M NaCl) is due to the effect of solvents on the chemical reactivity of purine residues, but does not reflect a conformational transition. The analysis of these results allows us to conclude, that alternating polynucleotides under the above mentioned conditions retain roughly the conformations inherent in them in 0.15 M NaCl: poly[d(A-C)].poly[d(G-T)] conformation in 4.3 m CsF or 60% ethanol differs only insignificantly from the "canonic" B-DNA, whereas the poly[d(A-T)].poly[d(A-T)] conformation in 6 M CSF corresponds to B-alternating DNA.     

Spectroscopic analysis of the interaction of Escherichia coli DNA-dependent RNA polymerase with T7 DNA and synthetic polynucleotides.

We have studied the circular dichroism and ultraviolet difference spectra of T7 bacteriophage DNA and various synthetic polynucleotides upon addition of Escherichia coli RNA polymerase. When RNA polymerase binds nonspecifically to T7 DNA, the CD spectrum shows a decrease in the maximum at 272 but no detectable changes in other regions of the spectrum. This CD change can be compared with those associated with known conformational changes in DNA. Nonspecific binding to RNA polymerase leads to an increase in the winding angle, theta, in T7 DNA. The CD and UV difference spectra for poly[d(A-T)] at 4 degrees C show similar effects. At 25 degrees C, binding of RNA polymerase to poly[d(A-T)] leads to hyperchromicity at 263 nm and to significant changes in CD. These effects are consistent with an opening of the double helix, i.e. melting of a short region of the DNA. The hyperchromicity observed at 263 nm for poly[d(A-T)] is used to determine the number of base pairs disrupted in the binding of RNA polymerase holoenzyme. The melting effect involves about 10 base pairs/RNA polymerase molecule. Changes in the CD of poly(dT) and poly(dA) on binding to RNA polymerase suggest an unstacking of the bases with a change in the backbone conformation. This is further confirmed by the UV difference spectra. We also show direct evidence for differences in the template binding site between holo- and core enzyme, presumably induced by the sigma subunit. By titration of the enzyme with poly(dT) the physical site size of RNA polymerase on single-stranded DNA is approximately equal to 30 bases for both holo- and core enzyme. Titration of poly[d(A-T)] with polymerase places the figure at approximately equal to 28 base pairs for double-stranded DNA.     

Evidence for Z-form RNA by vacuum UV circular dichroism.

Circular dichroism (CD) spectra in the vacuum UV region for different conformations of poly d(G-C) X poly d(G-C) and poly r(G-C) X poly r(G-C) are very characteristic. The CD of the RNA in the A-form (6 M NaClO4 and 22 degrees C) is very similar to that of the DNA in 80% alcohol where it is believed to be in the A-form. With the exception of the longest wavelength transition, the CD of the RNA in 6 M NaClO4 at 46 degrees C is similar to the CD of the DNA under conditions where it is believed to be in the Z-form (2 M NaClO4). This substantiates that poly r(G-C) X poly r(G-C) assumes a left-handed Z-conformation in 6 M NaClO4 above 35 degrees C. CD spectra for the left-handed Z-forms of both the RNA and DNA are characterized by an intense negative peak at 190-195 nm, a crossover at about 184 nm, and an intense positive peak below 180 nm. The right-handed A- and B-forms of RNA and DNA all have an intense positive peak in their CD spectra near 186 nm. The large difference in CD in the range 185-195 nm for right- and left-handed conformations of nucleic acids can be used to identify the sense of helix winding.     

Poly(2-amino-8-methyldeoxyadenylic acid): contrasting effects in deoxy- and ribopolynucleotides of 2-amino and 8-methyl substituents

Poly(2-amino-8-methyldeoxyadenylic acid) interacts readily with pyrimidine polynucleotides to form double helices only slightly less stable than those in which the purine polymer lacks the 8-Me group. In the ribo series, by contrast, complexes formed with poly(2-amino-8-methyladenylic acid) are very strongly destabilized by the 8-Me group, despite a larger stabilizing effect of the 2-NH2 group in the ribo series. These results are interpreted in terms of a smaller steric interference of the 8-Me group with 2'-CH2 than with 2'-CHOH, leading to a smaller population of syn structures in the deoxy chain and a consequent lower interference with homopolymer duplex formation. UV, circular dichroism (CD), and IR spectra of the new polymer and its complexes are reported and related to structural and energetic characteristics of the molecules. Since direct synthesis of 2-amino-8-methyldeoxyadenosine was not feasible, the corresponding riboside was prepared, the 3'- and 5'-positions were protected with a disilyloxy group, and a 2'-[(imidazol-1-yl)thiocarbonyl] group was introduced. Reduction with tributyltin hydride followed by deprotection gave the nucleoside, which was then converted to the triphosphate by standard methods. The homopolymer was prepared with terminal deoxynucleotidyl transferase.     

Intercalative and nonintercalative binding of large cationic porphyrin ligands to polynucleotides

The interactions of two positional isomers and one analogue of meso-tetra (4-N-methylpyridyl) porphine, with the synthetic polynucleotides poly[d(A-T)] . poly[d(A-T)] and poly[d(G-C)] . poly[d(G-C)] have been investigated by circular dichroism. All four porphyrins were found to bind to the polynucleotides as shown by the induction of circular dichroism in their Soret bands. Furthermore, the sign of the induced ellipticity reflects selective occupation of binding sites by the porphyrin ligands. The conformational lability of poly[d(A-T)] X poly[d(A-T)] was found to be appreciable as micromolar amounts of meso-substituted 4-N-methylpyridyl, 3-N-methylpyridyl, and p-N-trimethylanilinium porphines induced a CD spectrum similar but not identical to that of DNA in the Z-form, i.e. a negative band at 280 nm and a positive band at 259 nm. The effect of porphyrin binding to poly[d(G-C)] X poly[d(G-C)] was less pronounced and dissimilar to that seen in the AT polymer.     

The Escherichia coli O6-methylguanine-DNA methyltransferase does not repair promutagenic O6-methylguanine residues when present in Z-DNA

The repair of O6-methylguanine present in N-methylnitrosourea (MNU)-treated alternating polynucleotides MNU-poly(dG-dC) X poly(dG-dC) and MNU-poly(dG-me5dC) X poly(dG-me5dC] was investigated using O6-methylguanine-DNA methyltransferase purified from Escherichia coli. Both modified polynucleotides are equally good substrates for the DNA methyltransferase when they are in the B-form. The substrate properties of the MNU-treated polynucleotides do not differ from those of MNU-treated DNA. One of these modified polynucleotides, MNU-poly(dG-me5dC) X (dG-me5dC), can adopt the Z-conformation under physiological conditions. The conformational transition of the poly(dG-me5dC) X poly(dG-me5dC) from the B-form to the Z-form was monitored by the modification of its spectroscopic properties and by the specific binding of antibodies raised against Z-DNA. The O6-methylguanine residues are repaired in MNU-poly(dG-me5dC) X poly(dG-me5dC) in B-form. At variance, the conversion of this template to the Z-form completely inhibits the repair of the O6-methylguanine residues. The cooperative transition from the Z- to the B-form of MNU-poly(dG-me5dC) X poly(dG-me5dC), mediated by intercalating drugs such as ethidium bromide, restores the ability of MNU-poly(dG-me5dC) X poly(dG-me5dC) to be substrate for the transferase. These results imply that the promutagenic DNA lesion O6-methylguanine persists in Z-DNA fragments and suggest that DNA conformation modulates the extent of DNA repair and, as a result, plays an important role in determining the mutagenic potency of chemical carcinogens.     

Interaction of the HMG1 protein with nucleic acids

Binding constants have been measured for the interaction of the protein HMG1 with native DNA, denatured DNA and a number of polynucleotides at near-physiological ionic strengths, using gel filtration and thermal denaturation. The interaction of HMG1 with DNA is shown to be noncooperative and reversible. Nucleic acids form the following series in order of increasing binding constants: poly(U) integral of poly(A) less than poly(dA) less than dsDNA integral of poly(dA) X poly(dT) integral of poly(dG) X poly(dC) much less than poly[d(A-T]) integral of ssDNA.     

Optical rotatory dispersion and circular dichroism of silver(I):Polyribonucleotide complexes

Optical rotatory dispersion (ORD) and circular dichroism (CD) spectra of single- and multistranded polyribonucleotides undergo extensive changes on binding of the silver ion. These changes are consistent with the proposition that Ag(I) binds to the heterocyclic bases and not to the phosphate groups of polynucleotides. ORD and CD of silver complexes of poly(A)·poly(U) and double-helical rice dwarf viral RNA display negative Cotton effects when there is more than one Ag(I) per two nucleotide residues in solution. These observations suggest a significant distortion of the double-helical conformation as a result of Ag(I) binding. Silver(I) binding sites of pyrimidine polynucleotides are apparently saturated when there is one Ag(I) per two nucleotide residues and those of purine polynucleotides at one Ag(I) per nucleotide in solution. These data are consistent with the supposition that some Ag(I) binding sites exist on the pyrimidine ring and additional sites on the imidazole ring of polynucleotides. The sedimentation coefficient of poly(A) increases by severalfold when one Ag(I) is present per nucleotide residue. Silver(I) may introduce intra- and interstrand cross-links (through bidentate chelates) in single-stranded polynucleotides, resulting in structures with high sedimentation coefficients. Among the polynucleotides studied, poly(U) was an exception. Silver(I) did not affect the optical properties (absorbance, ORD, and CD) of poly(U) at neutral pH.     

Study of conformation characteristics of polydeoxyribonucleotides with non-random base sequence by slow 1H----3H exchange

The rate constants of 1H----3H exchange between water and C8H-groups of purinic residues of alternating polynucleotides: poly[d(A-T)].poly[d(A-T)] (I), poly[d(G-C)].poly[d(G-C)] (II), poly[d(A-C)].poly[d(G-T)] (III) and homopolynucleotides: poly(dA).poly(dt) (IV), poly(dG).poly(dC) (V), as well as DNA E. coli, was determined in 0.15 M NaCl at 25 degrees C. The retardation of exchange observed at these conditions (compared to that of the B-form DNA) is in agreement with the model of B-alternating structure for the (I) and is attributed to the co-existence of B- and A-conformers for the (V) in solution. Absence of distinguishable differences in exchange rate constants for purinic residues of the (II), (III) and (IV) (compared to that of the B-form DNA) evidences that conformations of these polynucleotides in solution are similar to "canonical" B-form DNA and don't correlate with the model of "heteronomous" DNA which was proposed for (IV).     

Carcinogenic purine N-oxide ester modifies covalently all common bases in polynucleotides

The carcinogen 1-methyl-3-hydroxyxanthine after esterification binds covalently to polynucleotides, RNA and DNA. All four ribopolynucleotides and poly(dT) are targets. Depending on reaction conditions, covalent binding is greatest to poly(A) followed by poly(U), poly(dT), poly(G), poly(C), RNA and DNA. Maximal covalent modification of DNA is one moiety per 360 nucleotides. All modified polynucleotides, RNA and DNA, except poly guanylic acid have been enzymatically digested and the major adducts characterized as nucleosides.     

Four-stranded DNA. Conformational analysis of regular spirals of poly(dT).poly(dA).poly(dA).poly(dT) with different base binding variations

Conformational analysis of four stranded DNA helices poly(dT).poly(dA).poly(dA).poly(dT) with parallel arrangement of the identical sugar-phosphate chains connected by twofold symmetry has been performed. All possible models of symmetrical base binding were checked. By the potential energy optimization the dihedral angles and helices parameters of stable conformations of four stranded polynucleotides were calculated. The dependences of conformational energy on the base complex structure and mutual orientation of the poly(dA).and poly(dT) chains were studied. Possible biological functions of four stranded helices are discussed.     

Covalent binding of benzo[a]pyrenediol epoxides to polynucleotides

Spectroscopic studies on the trans-7,8-dihydroxy-anti-9,10-epoxy-7,8,9,10-tetrahydrobenzo[a]pyrene- (anti-BPDE-) modified synthetic polynucleotide solutions reveal interesting sequence-dependent stereoselective covalent binding of anti-BPDE to DNA. Absorption spectral results indicate that the G.C polymers are much more reactive than the A.T polymers toward this metabolite and the homopolymer suffers higher modification than its corresponding alternating polynucleotide. The covalently attached anti-BPDE exhibits only a 2-3-nm red shift in the guanine-containing polynucleotide and native DNA solutions as opposed to the 8-nm red shift in poly(G) and none in the A.T polymers. Distinct stereoselectivities are exhibited by poly(dG-dC).poly(dG-dC) vs. poly(dG).poly(dC) as suggested by the oppositely signed CD in the pyrene spectral region. Comparison with the syn-BPDE modified polynucleotides reveals some interesting differences with its anti diastereomer. Significant contributions from the intercalated syn-BPDE are apparent in the modified guanine-containing polynucleotides as indicated by the appearance of 10-nm red-shifted shoulders. In contrast to the strong dependence on polynucleotides for anti-BPDE, the rate of hydrolysis of syn-BPDE appears to be insensitive to their presence in the solution. anti-BPDE modification on the 50 microM hexaamminecobalt-induced Z-form poly(dG-dC).poly(dG-dC) is much less extensive than its corresponding B form, possibly the consequence of both structural and ionic strength factors. The spectral characteristics of anti-BPDE bonded to these two forms are distinctly different, with the Z form resembling more closely those of A.T polymers.(ABSTRACT TRUNCATED AT 250 WORDS)     

Parallel double DNA spiral. A conformational analysis of regular spirals of poly(dA).poly(dT) with different variations of joining bases

We have performed a conformational analysis of DNA double helices poly(dA).poly(dT) with parallel directed backbone strands in heteronomic model frames. All possible models of base pairs and various mutual orientation of base pair and sugarphosphate backbones were checked. By the potential energy optimization the dihedral angles and helices parameters of stable conformations of parallel double polynucleotides were calculated. The dependences of conformational energy on the base pair structure were studied.     

Parallel DNA helices. Conformational analysis of regular poly(dG).poly(dC) helices with different variants of base binding]

We have performed a conformational analysis of DNA double helices with parallel directed backbone strands. The calculations were made for homopolymers poly(dG).poly(dC). All possible models of base binding were checked. By the potential energy optimization the dihedral angles and helices parameters of stable conformations of parallel double polynucleotides were calculated. The dependences of conformational energy on the base pair structure were studied. Possible structure of parallel helices with various nucleotide composition are discussed.     

Nucleotide sequence-dependent opening of double-stranded DNA at an electrically charged surface

It has been shown earlier that the DNA double helix is opened due to a prolonged contact of the DNA molecule with the surface of the mercury electrode. At neutral pH, the opening process is relatively slow (around 100 s), and it is limited to potentials close to -1.2 V (against SCE). The opening of the double helix has been explained by strains in the DNA molecule due to strong repulsion of the negatively charged phosphate residues from the electrode surface where the polynucleotide chain is anchored via hydrophobic bases. Interaction of the synthetic ds polynucleotides with alternating nucleotide sequences/poly(dA-dT).poly (dA-dT), poly (dA-dU).poly (dA-dU), poly (dG-dC).poly (dG-dC)/ and homopolymer pairs/poly (dA).poly (dT), poly (rA).poly (rU) and poly (dG).poly (dC)/ with the hanging mercury drop electrode has been studied. Changes in reducibility of the polynucleotides were exploited to indicate opening of the double helix. A marked difference in the behaviour was observed between polynucleotides with alternating nucleotide sequence and homopolymer pairs: opening of the double-helical structures of the former polynucleotides occurs at a very narrow potential range (less than 100 mV) (region U), while with the homopolymer pairs containing A X T or A X U pairs, the width of this region is comparable to that of natural DNA (greater than 200 mV). In contrast to natural DNA, the region U of homopolymer pairs is composed of two distinct phases. No region U was observed with poly (dG).poly (dC). In polynucleotides with alternating nucleotide sequence, the rate of opening of the double helix is strongly dependent on the electrode potential in region U, while in homopolymer pairs, this rate is less potential-dependent. It has been assumed that the difference in the behaviour between homopolymer pairs and polynucleotides with alternating nucleotide sequence is due to differences in absorbability of the two polynucleotide chains in the molecule of a homopolymer pair (resulting from different absorbability of purine and pyrimidine bases) in contrast to equal adsorbability of both chains in a polynucleotide molecule with alternating nucleotide sequence. It has been shown that the mercury electrode is a good model of biological surfaces (e.g. membranes), and that the nucleotide sequence-dependent opening (unwinding) of the DNA double helix at electrically charged surfaces may play an important role in many biological processes.     

Study of the binding of single-stranded DNA-binding protein to DNA and poly(rA) using electric field induced birefringence and circular dichroism spectroscopy

Binding of the single-stranded DNA-binding protein (SSB) of Escherichia coli to single-stranded (ss) polynucleotides produces characteristic changes in the absorbance (OD) and circular dichroism (CD) spectra of the polynucleotides. By use of these techniques, complexes of SSB protein and poly(rA) were shown to display two of the binding modes reported by Lohman and Overman [Lohman, T.M., & Overman, L. (1985) J. Biol. Chem. 260, 3594-3603]. The circular dichroism spectra of the "low salt" (10 mM NaCl) and "high salt" (greater than 50 mM NaCl) binding mode are similar in shape, but not in intensity. SSB binding to poly(rA) yields a complexed CD spectrum that shares several characteristics with the spectra obtained for the binding of AdDBP, GP32, and gene V protein to poly(rA). We therefore propose that the local structure of the SSB-poly(rA) complex is comparable to the structures proposed for the complexes of these three-stranded DNA-binding proteins with DNA (and RNA) and independent of the SSB-binding mode. Electric field induced birefringence experiments were used to show that the projected base-base distance of the complex is about 0.23 nm, in agreement with electron microscopy results. Nevertheless, the local distance between the successive bases in the complex will be quite large, due to the coiling of the DNA around the SSB tetramer, thus partly explaining the observed CD changes induced upon complexation with single-stranded DNA and RNA.     

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.