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.     

Four-stranded DNA helices: conformational analysis of regular poly(dT).poly(dA).poly(dA).poly(dT) helices with various types of base binding

The paper presents results obtained in conformational analysis of homopolymeric four-stranded poly(dT).poly(dA).poly(dA).poly(dT) DNA helices in which the pairs of strands with identical bases are parallel and have a two-fold symmetry axis. All possible models of base binding to yield a symmetric complex have been considered. The dihedral angles of sugar-phosphate backbones and helix parameters, which are consistent with the minima of conformational energy for four-stranded DNAs, have been determined using the results of optimization of conformational energy calculated at atom-atom approximation. Potential energy is shown to depend on the structure of base complexes and on the mutual orientation of unlike strands. Possible biological functions of four-stranded helices are discussed.     

Structure of poly (I).poly (A).poly (I)

The molecular structure of poly (I).poly (A).poly (I) has been determined and refined using the continuous intensity data on layer lines in the x-ray diffraction pattern obtained from an oriented fiber of this polymorphic RNA complex. The polymer forms a 12-fold right-handed triple-helix of pitch 39.7A and each base-triplet is stabilized by quasi Crick-Watson-Hoogsteen hydrogen bonds. The ribose rings in all the three strands have C3'-endo conformations. The final R-value for this best structure is 0.24 and the x-ray fit is significantly superior to all the alternative structures where the different chains might have different furanose conformations. This all-purine triple-helix, counter-intuitively, has a diameter roughly 3A shorter than that of DNA and RNA triple-helices containing a homopurine and two complementary homopyrimidine strands. Its compact, grooveless cylindrical shape is consistent with the lack of lateral organization.     

Structure of Poly (U).poly (A).poly (U)

The molecular structure of poly (U).poly (A).poly (U) has been determined and refined using the continuous x-ray intensity data on layer lines in the diffraction pattern obtained from an oriented fiber of the RNA. The final R-value for the preferred structure is 0.24, far lower than that for the plausible alternatives. The polymer forms an 11-fold right-handed triple-helix of pitch 33.5A and each base triplet is stabilized by Crick-Watson-Hoogsteen hydrogen bonds. The ribose rings in the three strands have C3'-endo, C2'-endo and C2'-endo conformations, respectively. The helix derives additional stability through systematic interchain hydrogen bonds involving ribose hydroxyls and uracil bases. The relatively grooveless cylindrical shape of the triple-helix is consistent with the lack of lateral organization.     

Unique poly(dA).poly(dT) B'-conformation in cellular and synthetic DNAs

Poly(dA).poly(dT), but not B-form DNA, is specifically recognized by experimentally induced anti-kinetoplast or anti-poly(dA).poly(dT) immunoglobulins. Antibody binding is completely competed by poly(dA).poly(dT) and poly(dA).poly(dU) but not by other single- or double-stranded DNA sequences in a right-handed B-form. Antibody interaction with poly(dA).poly(dT) depends on immunoglobulin concentration, incubation time and temperature, and is sensitive to elevated ionic strengths. Similar conformations, for example, (dA)4-6 X (dT)4-6, in the kinetoplast DNA of the parasite Leishmania tarentolae are also immunogenic and induce specific anti-poly(dA).poly(dT) antibodies. These antibody probes specifically recognize nuclear and kinetoplast DNA in fixed flagellated kinetoplastid cells as evidenced by immunofluorescence microscopy. Anti-poly(dA).poly(dT) immunofluorescence is DNase-sensitive and competed by poly(dA).poly(dT), but not other classical double-stranded B-DNAs. Thus, these unique cellular B'-DNA helices are immunogenic and structurally similar to synthetic poly(dA).poly(dT) helices in solution.     

Structure of poly(dA).poly(dT) is not identical to the AT rich regions of the single crystal structure of CGCGAATTBrCGCG. The consequence of this to netropsin binding to poly(dA).poly(dT)

The basic assumption of Dickerson and Kopka (J. Biomole. Str. Dyns. 2, 423, 1985) that the conformation of poly(dA).poly(dT) in solution is identical to the AT rich region of the single crystal structure of the Dickerson dodecamer is not supported by any experimental data. In poly(dA).poly(dT), NOE and Raman studies indicate that the dA and dT units are conformationally equivalent and display the (anti-S-type sugar)-conformation; incorporation of this nucleotide geometry into a double helix leads to a conventional regular B-helix in which the width of the minor groove is 8A. The derived structure is consistent with all available experimental data on poly(dA).poly(dT) obtained under solution conditions. In the crystal structure of the dodecamer, the dA and dT units have distinctly different conformations-dA residues adopt (anti, S-type sugar pucker), while dT residues belong to (low anti, N-type sugar pucker). These different conformations of the dA and dT units along with the large propeller twist can be accommodated in a double helix in which the minor groove is shrunk from 8A to less than 4A. In the conventional right handed B-form of poly(dA).poly(dT) with the 8A wide minor groove, netropsin has to bind asymmetrically along the dA strand to account for the NOE and chemical shift data and to generate a stereochemically sound structure (Sarma et al, J. Biomole. Str. Dyns. 2, 1085, 1985).     

The propeller DNA conformation of poly(dA).poly(dT).

Physical properties of the DNA duplex, poly(dA).poly(dT) differ considerably from the alternating copolymer poly(dAT). A number of molecular models have been used to describe these structures obtained from fiber X-ray diffraction data. The recent solutions of single crystal DNA dodecamer structures with segments of oligo-A.oligo-T have revealed the presence of a high propeller twist in the AT regions which is stabilized by the formation of bifurcated (three-center) hydrogen bonds on the floor of the major groove, involving the N6 amino group of adenine hydrogen bonding to two O4 atoms of adjacent thymine residues on the opposite strand. Here we show that it is possible to incorporate the features of the single crystal analysis, specifically high propeller twist, bifurcated hydrogen bonds, and a narrow minor groove, as well as the close interstrand NMR signal between adenine HC2 and ribose HC1' of the opposite strand, into a model that is fully compatible with the diffraction data obtained from poly(dA).poly(dT).     

Complete disproportionation of duplex poly(dT)*poly(dA) into triplex poly(dT)*poly(dA)*poly(dT) and poly(dA) by coralyne

Coralyne is a small crescent-shaped molecule known to intercalate duplex and triplex DNA. We report that coralyne can cause the complete and irreversible disproportionation of duplex poly(dT)·poly(dA). That is, coralyne causes the strands of duplex poly(dT)·poly(dA) to repartition into equal molar equivalents of triplex poly(dT)·poly(dA)·poly(dT) and poly(dA). Poly(dT)·poly(dA) will remain as a duplex for months after the addition of coralyne, if the sample is maintained at 4°C. However, disproportionation readily occurs upon heating above 35°C and is not reversed by subsequent cooling. A titration of poly(dT)·poly(dA) with coralyne reveals that disproportionation is favored by as little as one molar equivalent of coralyne per eight base pairs of initial duplex. We have also found that poly(dA) forms a self-structure in the presence of coralyne with a melting temperature of 47°C, for the conditions of our study. This poly(dA) self-structure binds coralyne with an affinity that is comparable with that of triplex poly(dT)·poly(dA)·poly(dT). A Job plot analysis reveals that the maximum level of poly(dA) self-structure intercalation is 0.25 coralyne molecules per adenine base. This conforms to the nearest neighbor exclusion principle for a poly(dA) duplex structure with A·A base pairs. We propose that duplex disproportionation by coralyne is promoted by both the triplex and the poly(dA) self-structure having binding constants for coralyne that are greater than that of duplex poly(dT)·poly(dA).     

The structure of poly(dA).poly(dT) as revealed by an X-ray fibre diffraction

X-ray diffraction in fibres revealed that the calcium salt of poly(dA).poly(dT) is a 10-fold double helix with a pitch of 3.23 nm. The opposite sugar-phosphate chains in the refined model are characterized by a complete conformational equivalence and contain sugars in a conformation close to C2'-endo. As a result a new model of the sodium salt of poly(dA).poly(dT) has been constructed, which is different from the Heteronomous DNA proposed earlier (S. Arnott et al., Nucl. Acids Res. 11, 4141 (1983)). The new model of Na-poly(dA).poly(dT) has conformationally similar opposite chains; it is a structure of the B-type, rather like that of Ca-poly(dA).poly(dT).     

1H two-dimensional nuclear Overhauser effect and relaxation studies of poly(dA).poly(dT)

The structure of poly(dA).poly(dT) in aqueous solution has been studied by using 1H two-dimensional nuclear Overhauser effect (2D NOE) spectroscopy and relaxation rate measurements on the imino and nonexchangeable protons. The assignments of the 1H resonances are determined from the observed cross-relaxation patterns in the 2D NOE experiments. The cross-peak intensities together with the measured relaxation rates show that the purine and pyrimidine strands in poly(dA).poly(dT) are equivalent in aqueous solution. The results are consistent with a right-handed B-form helix where the sugars on both strands are in the C2'-endo/anti configuration. These observations are inconsistent with a proposed heteronomous structure for poly(dA).poly(dT) [Arnott, S., Chandrasekaran, R., Hall, I. H., & Puigjaner, L. C. (1983) Nucleic Acids Res. 11, 4141-4155]. The measured relaxation rates also show that poly(dA).poly(dT) has fast, large-amplitude local internal motions (+/- 20-25 degrees) in solution and that the amplitudes of the base and sugar motions are similar. The motion of the bases in poly(dA).poly(dT) is also similar to that previously reported for poly(dA-dT).poly(dA-dT) and poly(dG-dC).poly(dG-dC) [Assa-Munt, N., Granot, J., Behling, R. W., & Kearns, D. R. (1984) Biochemistry 23, 944-955; Mirau, P. A., Behling, R. W., & Kearns, D. R. (1985) Biochemistry 24, 6200-6211].     

Poly(dA).poly(dT) exists in an unusual conformation under physiological conditions: propidium binding to poly(dA).poly(dT) and poly[d(A-T)].poly[d(A-T)]

The binding of propidium to poly(dA).poly(dT) [poly(dA.dT)] and to poly[d(A-T)].poly[d(A-T)] [poly[d(A-T)2]] has been compared under a variety of solution conditions by viscometric titrations, binding studies, and kinetic experiments. The binding of propidium to poly[d(A-T)2] is quite similar to its binding to calf thymus deoxyribonucleic acid (DNA). The interaction with poly(dA.dT), however, is quite unusual. The viscosity of a poly(dA.dT) solution first decreases and then increases in a titration with propidium at 18 degrees C. The viscosity of poly[d(A-T)2] shows no decrease in a similar titration. Scatchard plots for the interaction of propidium with poly(dA.dT) show the classical upward curvature for positive cooperativity. The curvature decreases as the temperature is increased in binding experiments. A van't Hoff plot of the observed binding constants yields an apparent positive enthalpy of approximately +6 kcal/mol for the propidium-poly(dA.dT) interaction. Propidium binding to poly[d(A-T)2] shows no evidence for positive cooperativity, and the enthalpy change for the reaction is approximately -9 kcal/mol. Both the magnitude of the dissociation constants and the effects of ionic strength are quite similar for the dissociation of propidium from poly(dA-T)2] and from poly[d(A-T)2], suggesting that the intercalated states are similar for the two complexes. The observed association reactions, under pseudo-first-order conditions, are quite different. Plots of the observed pseudo-first-order association rate constant vs. polymer concentration have much larger slopes for propidium binding to poly[d(A-T)2] than to poly(dA.dT).(ABSTRACT TRUNCATED AT 250 WORDS)     

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

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

Structure of poly(dA).poly(dT) from data of x-ray diffraction, energy calculations and nuclear magnetic resonance

The results of X-ray diffraction studies of poly(dA).poly(dT) have been compared with the results of energy optimization and with the NMR data in solution. Slight refinement of the X-ray and energetically optimal models leads to a very good quantitative agreement with the NMR data, that suggests similarity of the poly(dA).poly(dT) structure in a condensed state and in solution. One of the features distinguishing these models from the classic B form is a narrowed minor groove of the double helix. The anomalous properties of DNA with this sequence can be related specific organization of the water molecules near the polynucleotide.     

DNA with adenine tracts contains poly(dA).poly(dT) conformational features in solution.

The conformation of DNA's with adenine-thymine tracts exhibiting retardation in electrophoretic migration and considered as curved were investigated in solution by CD and RAMAN spectroscopy. The following curved multimers with adenine tracts but of different flanking sequences d(CA5TGCC)n, d(TCTCTA6TATATA5)n, d(GA4T4C)n yield CD spectroscopic features indicating a non-B structure of the dA.dT tract with similarities to polyd(A).polyd(T). We suggest that adenine-thymine bases in these multimers contain some of the distinctive conformational features of poly(A).polyd(T) probably with large propeller twist found by NMR (Behling and Kearns, 1987) and by X-ray diffraction on oligonucleotides containing a tract of adenines (Nelson et al. 1987, Coll et al; 1987; DiGabriele et al. 1989). Some elements of distinctive CD features of the contiguous adenines run are also observed in the straight multi-9-mer d(CA5GCC)n which lacks in-phase relation to the helical repeat. Despite the presence of the TpA step in the straight multimer d(GT4A4)n, the altered dA.dT conformation is not completely destroyed. Interruption of adenine tract by a guanine in d(CAAGAATGCC)n leads to a B-like conformation and to a normal electrophoretic mobility. The Raman spectra reveal a rearrangement of the sugar-phosphate backbone of dA.dT tract in the multimer d(CA5TGCC)n with respect to that of polydA.polydT. This is reflected in the presence of an unique Raman band associated to C2'-endo sugar with a predominant contribution of C1'-exo puckering which is exhibited by the multimer whereas two distinct Raman bands characterize poly(dA).poly(dT) backbone conformation.     

Poly(dA).poly(dT) rich sequences are not sufficient to exclude nucleosome formation in a constitutive yeast promoter.

It was suggested that poly(dA).poly(dT) rich sequences in yeast Saccharomyces cerevisiae act as elements of constitutive promoters by exclusion of nucleosomes (Struhl, K. (1985). Proc. Natl. Acad. Sci. USA 82, 8419-8423). We have mapped the chromatin structure of the pet56-his3-ded1 region in minichromosomes and show that the poly(dA).poly(dT) sequences are located in nuclease sensitive regions. DNA fragments from the nuclease sensitive promoter region of DED1 were used for nucleosome reconstitution in vitro. We show that all sequences can form nucleosome cores and that the poly(dA).poly(dT) sequence can be incorporated in nucleosome cores. The results suggest that the nuclease sensitivity found in vivo is not established by poly(dA).poly(dT) mediated exclusion of nucleosomes.     

High pressure fourier transform infrared spectroscopy of poly(dA)poly(dT), poly(dA) and poly(dT)

The effect of hydrostatic pressure upon the DNA duplex, poly(dA)poly(dT), and its component single strands, poly(dA) and poly(dT) has been studied by fourier-transform infrared spectroscopy (FT-IR). The spectral data indicate that at 28 degrees C and pressures up to 12 kbar (1200 MPa) all three polymers retain the B conformation. Pressure causes the band at 967 cm(-1), arising from water-deoxyribose interactions, to shift to higher frequencies, a result consistent with increased hydration at elevated pressures. A larger pressure-induced frequency shift in this band is observed in the single stranded polymers than in the double stranded molecule, suggesting that the effect of pressure on the hydration of single strands may be greater than upon a double stranded complex. A pressure-dependent hypochromicity in the bands attributed to base stacking indicates that pressure facilitates the base stacking in the three polymers, in agreement with previous assessments of the importance of stacking in the stabilization of DNA secondary structure at ambient and high pressures.     

Acoustical investigation of poly(dA).poly(dT), poly[d(A-T)], poly(A).poly(U) and DNA hydration in dilute aqueous solutions.

Apparent molar adiabatic compressibilities and apparent molar volumes of poly[d(A-T)].poly[d(A-T)], poly(dA).poly(dT), DNA and poly(A).poly(U) in aqueous solutions were determined at 1 degree C. The change of concentration increment of the ultrasonic velocity upon replacing counter ion Cs+ by the Mg2+ ion was also determined for these polymers. The following conclusions have been made: (1) the hydration of the double helix of poly(dA).poly(dT) is remarkably larger than that of other polynucleotides; (2) the hydration of the AT pair in the B-form DNA is larger than that of the GC pair; (3) the substitution of Cs+ for Mg2+ ions as counter ions results in a decrease of hydration of the system polynucleotide plus Mg2+, and (4) the magnitude of this dehydration depends on the nucleotide sequence; the following rule is true: the lesser is a polynucleotide hydration, the larger dehydration upon changing Cs+ for Mg2+ ions in the ionic atmosphere of polynucleotide.     

Nucleosomes will not form on double-stranded RNa or over poly(dA).poly(dT) tracts in recombinant DNA.

We have been unable to "force" double-stranded RNA to fold into nucleosome-like structures using several different histone-RNA "reconstitution" procedures. Even if the histones are first stabilized in octameric form by dimethylsuberimidate cross-linking they are still unable to form specific complexes with the RNA. Moreover double-stranded RNA is unable to induce histones to assemble into octamers although we confirm that the non-nucleic acid homopolymer, polyglutamic acid, has this ability. We have also determined, using pyrimidine tract analysis, that nucleosomes will not form over a sufficiently long segment of poly(dA).poly(dT) in a recombinant DNA molecule. Thus nucleosomes cannot fold DNA containing an 80 base pair poly(dA).poly(dT) segment but a 20 base pair segment can be accommodated in nucleosomes fairly well. Segments of intermediate length can be accommodated but are clearly selected against. Poly(dA).poly(dT) differs only slightly from natural DNA in helix structure. Therefore either this homopolymer resists folding, or nucleosomes are very exacting in the nucleic acid steroid parameters they will tolerate. Such constraints may be relevant to nucleosome positioning in chromatin.     

A unique deletion in pBR322 DNA caused by insertion of poly(dA).poly(dT)

A unique deletion covering around 43% of the pBR322 genome was found after attempting to insert 100 or 200 bp poly(dA).poly(dT) into the EcoRV site of pBR322 DNA. This result was not observed if an equivalent size heterologous DNA or a larger poly(dA).poly(dT) fragment of 10-20,000 bp was introduced at the same site. DNA sequencing analysis at the junctions suggests that a specific intramolecular pairing may be involved in the formation of this deletion mutant.