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.     

Poly(dG).poly(dC) at neutral and alkaline pH: the formation of triple stranded poly(dG).poly(dG).poly(dC).

Alkaline titrations of different samples of poly(dG).poly(dC) and of the constituent homopolymers poly(dG) and poly(dC) have been performed in 0.15 M NaCl and their CD spectra followed. Sample I contained a slight excess of poly(dC) (52% C: 48% G) and showed a single reversible transition (pK = 11.9) due to the dissociation of double stranded poly(dG).poly(dC). Sample II, containing an excess of poly(dG) (43% C: 57% G), showed two transitions (pK1 = 11.4, PK2 = 11.9) the first one being only partially reversible. Examination of the CD spectra along the alkaline titrations indicated the presence of another hydrogen-bonded complex of higher G content. Mixing curves performed at pH 8 have confirmed the presence of a 2G: 1C complex, besides the double stranded complex. It can be formed in amounts up to 30% by mixing the two homopolymers, alkali treatment and heating. The CD spectra of the two complexes have been computed from the CD data of the mixing curves. This permitted the determination of the concentrations of both complexes and homopolymers in all samples. The ratio of triple to double stranded complex is not only dependent on the G/C ratio of the sample, but also a function of the previous physico-chemical conditions. These results explain the variability of many properties of different poly(dG).poly(dC) samples observed by other workers.     

Binding mode of 4',6-diamidino-2-phenylindole and ethidium to poly(dG).poly(dC).poly(dC)(+) triplex and poly(dG).poly(dC) duplex

Optical spectroscopic properties of 4',6-diamidino-2-phenylindole (DAPI) and ethidium bromide complexed with poly(dG).poly(dC).poly(dC)(+) triplex and poly(dG).poly(dC) duplex were compared in this study. When complexed with both duplex and triplex, ethidium is characterized by hypochromism and a red shift in the absorption spectrum, a complicate induced circular dichroism (CD) band in the polynucleotide absorption region, and a negative reduced linear dichroism signal in both polynucleotide and drug absorption regions. The spectral properties for both duplex- and triplex-bound ethidium are identical and both can be understood by the intercalation binding mode. In contrast, the absorption and CD spectra of DAPI complexed with triplex differ from those of the DAPI-duplex complex, although both complexes can be understood by the intercalation binding mode. Considering that the third strand runs along the major groove of the template duplex, we conclude that the DAPI molecule partially intercalates near the major groove of the duplex, where the third strand can affect its spectroscopic properties.     

Parallel double helices of DNA. Conformational analysis of regular helices with the second order symmetry axis

We have performed a conformational analysis of DNA double helices with parallel directed backbone strands connected with the second order symmetry axis being at the same time the helix axis. The calculations were made for homopolymers poly(dA).poly(dA), poly(dC).poly(dC), poly(dG) poly(dG), and poly(dT).poly(dT). All possible variants of hydrogen bonding of base pairs of the same name were studied for each polymer. The maps of backbone chain geometrical existence were constructed. Conformational and helical parameters corresponding to local minima of conformational energy of "parallel" DNA helices, calculated at atom-atom approximation, were determined. The dependence of conformational energy on the base pair and on the hydrogen bond type was analysed. Two major conformational advantageous for "parallel" DNA's do not depend much on the hydrogen-bonded base pair type were indicated. One of them coincided with the conformational region typical for "antiparallel" DNA, in particular for the B-form DNA. Conformational energy of "parallel" DNA depends on the base pair type and for the most part is similar to the conformational energy of "antiparallel" B-DNA.     

The molecular electrostatic potential and steric accessibility of poly (dI.dC). Comparison with poly (dG.dC)

The influence of the amino group of guanine on the molecular electrostatic potential and the accessibility to reactive sites of B-DNA is investigated by comparing the two model double helices poly (dI.dC) and poly (dG.dC). The calculations clarify the “disruptive” role of the guanine amino group on nucleic acid-polypeptide interactions.     

Description of base motion and role of excitations in the melting of poly(dG).poly(dC).

We study the contribution of various vibrational modes to the melting of poly(dG).poly(dC). We find that the principal contribution comes from the H-bond breathing modes that have been observed in Raman scattering and that we have associated with helix melting. We show the softening of these modes on approach to melting in agreement with the observed behavior. We also describe the contribution to melting from base rotation modes that others have suggested are important in melting.     

Nucleosome reconstitution of core-length poly(dG).poly(dC) and poly(rG-dC).poly(rG-dC)

The double-stranded polypurine.polypyrimidines poly(dG).poly(dC) and poly[d(A-G)].poly[d(T-C)] and the mixed ribose-deoxyribose polynucleotide poly(rG-dC).poly(rG-dC) have been successfully reconstituted into nucleosomes. The radioactively labeled particles comigrate in gel electrophoresis and sucrose density gradient experiments with authentic nucleosomes derived from chicken erythrocyte chromatin. These results show that nucleosomes are able to accommodate a wider variety of polynucleotides than was previously believed.     

Conformational lability of poly(dG-m5dC):poly(dG-m5dC).

The remarkable conformational lability of poly(dG-m5dC):poly(dG-m5dC) is demonstrated by the observation of an acid-mediated conformational hysteresis. An acid-mediated Z conformation that exists in solutions containing low sodium concentrations that would normally favor the B conformation is described in this report. This Z conformation is reached by an acid-base titration of a B-poly(dG-m5dC):poly(dG-m5dC) solution which is not far from the B-Z transition midpoint. The resulting Z conformation is thermally very stable, with direct melting into single strands at approximately 100 degrees C. In contrast, the B form DNA, initially in solutions of the same ionic strength but without exposure to acidic pH, exhibits a biphasic melting profile, with conversion into the Z form (with high cooperativity) prior to an eventual denaturation into single strands at around 100 degrees C. Cooling experiments reveal that such biphasic transitions are quite reversible. The transition midpoint for the thermally poised B to Z transformation depends strongly on the NaCl concentration and varies with sample batch. The acid-mediated Z form binds ethidium more weakly than its B counterpart, and the ethidium induced Z to B conversion occurs in a step-wise (non-allosteric) fashion without the requirement of a threshold concentration. The acid-mediated as well as the thermally poised Z conformations are reversed by the addition of EDTA, suggesting the involvement of trace amounts of multivalent metal ions.     

Parallel DNA double helices. II. Conformational analysis of regular helices having a second order axis of symmetry

Conformational analysis of double helices of DNA with parallel arranged sugar-phosphate chains connected by twofold symmetry has been performed. Homopolymers poly(dA).poly(dA), poly(dC).poly(dC), poly(dG).poly(dG) and poly(dT).poly(dT) were studied. For each of the homopolymers all variants of H-bond pairing were checked. The maps of closing of sugar-phosphate backbone were previously computed. By the optimization of potential energy the dihedral angles and helix parameters of relatively stable conformations of parallel stranded polynucleotides were calculated. The dependence of conformational energy on the nucleic base character and the base pair type were studied. Two main conformational regions for favourable "parallel" helix of polynucleotides were found. The former of these two regions coincide with the region of typical conformational parameters of B-DNA. On an average the conformational energy of "parallel" DNA is close to the energy of canonic "antiparallel" B-DNA.     

Protonated polynucleotides structures - 23. The acid-base hysteresis of poly(dG).poly(dC).

The large hysteresis observed during the acid-base titration of poly(dG). poly (dC) was studied by CD and potentiometric scanning curves. Intermediate scanning loops as well as the equilibrium and metastable branches of the hysteresis loop have been determined. The potentiometric titrations showed, however, that the various complexes were not discrete entities, but were linked in "polycomplexes" as had been already suggested. This prevented a thermodynamic study of the system. The acid-base titration was further investigated as a function of ionic strength and temperature. The pK's showed considerably lower ionic strength dependence than observed for polyribonucleotide complexes. The thermal transitions permitted to establish the relative stabilities of the various complexes between pH 2.5 and pH 12.0.     

DNA in phosphorus atom representation: the heteronomous double helices of poly(dA).poly(dT) and poly(dG).poly(dC) and simulation of the yeast genome and of a human chromosome DNA

We extracted phosphorus atom coordinates from the database of DNA crystal structures and calculated geometrical parameters needed to reproduce the crystal structures in the phosphorus atom representation. Using the geometrical parameters we wrote a piece of software assigning the phosphorus atom coordinates to the DNA of any nucleotide sequence. The software demonstrates non-negligible influence of the primary structure on DNA helicity, which may stand behind the heteromonous double helices of poly(dA).poly(dT) and poly(dG).poly(dC). In addition, the software is so simple that it makes possible to simulate the "crystal" structures of not only viral DNAs, but also the whole genome of Saccharomyces cerevisiae as well as the DNA human chromosome 22 having dozens of megabases in length.     

The crystal structure of d(G-G-G-G-C-C-C-C). A model for poly(dG).poly(dC)

The structure of the DNA oligomer d(G-G-G-G-C-C-C-C) has been determined at a resolution of 2.5 A by single-crystal X-ray methods. There are two strands in the asymmetric unit, and these coil about each other to form a right-handed double-helix of the A-type with Watson-Crick hydrogen bonds between base-pairs. The helix has a shallow minor groove and a deep, water-filled major groove; almost all exposed functional groups on the DNA are hydrated, and 106 ordered solvent molecules have been found. The two d(G-G-G-G).d(C-C-C-C) segments in the octamer exhibit similar and uniform structures, but there is a slight discontinuity at the GpC step between them. A recurring feature of the structure is the overlap of adjacent guanine bases in each GpG step, with the five-membered ring of one guanine stacking on the six-membered ring of its neighbour. There is little or no overlap between adjacent cytosine rings. Conformational parameters for these GpG steps are compared with those from other single-crystal X-ray analyses. In general, GpG steps exhibit high slide, low roll and variable twist. Models for poly(dG).poly(dC) were generated by applying a simple rotation and translation to each of the unmodified d(G-G-G-G).d(C-C-C-C) units. Detailed features of these models are shown to be compatible with various assays of poly(dG).poly(dC) in solution, and are useful in understanding the polymorphic behaviour of this sequence under a variety of experimental conditions.     

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.     

Protonated polynucleotide structures, 20. Interaction between poly(dG)-poly(dC) and poly(rC).1.

A study of the interaction between poly(dG)-poly(dC) and poly(rC) demonstrates that, at neutral pH and high ionic strength, there is replacement of the dC strand by poly(rC). At acid pH, formation of a triple-stranded complex which equally may involve the replacement phenomenon is observed. There is no evidence for interaction at neutral pH between poly(dG)-poly(dC) and oligo(rC), while a three-stranded complex is formed at acid pH. These data are consistent with the studies of comparative stabilities of double stranded deoxy or ribo polymers and deoxy-ribo hybrids.     

Protonated polynucleotides structures - 22.CD study of the acid-base titration of poly(dG).poly(dC)

The acid-base titration (pH 8 --> pH 2.5 --> pH 8) of eleven mixing curve samples of the poly(dG) plus poly(dC) system has been performed in 0.15 M NaCl. Upon protonation, poly(dG).poly(dC) gives rise to an acid complex, in various amounts according to the origin of the sample. We have established that the hysteresis of the acid-base titration is due to the non-reversible formation of an acid complex, and the liberation of the homopolymers at the end of the acid titration and during the base titration: the homopolymer mixtures remain stable up to pH 7. A 1G:1C stoichiometry appears to be the most probable for the acid complex, a 1G:2C stoichiometry, as found in poly(C(+)).poly(I).poly(C) or poly(C(+)).poly(G).poly(C), cannot be rejected. In the course of this study, evidence has been found that the structural consequences of protonation could be similar for both double stranded poly(dG).poly(dC) and G-C rich DNA's: 1) protonation starts near pH 6, dissociation of the acid complex of poly(dG).poly(dC) and of protonated DNA take place at pH 3; 2) the CD spectrum computed for the acid polymer complex displays a positive peak at 255 nm as found in the acid spectra of DNA's; 3) double stranded poly(dG).poly(dC) embedded in triple-stranded poly(dG).poly(dG).poly(dC) should be in the A-form and appears to be prevented from the proton induced conformational change. The neutral triple stranded poly(dG).poly(dG).poly(dC) appears therefore responsible, although indirectly, for the complexity and variability of the acid titration of poly(dG).poly(dC) samples.     

Protonated forms of poly[d(G-C)] and poly(dG).poly(dC) and their interaction with berberine

The pH -induced structural changes on the conformation of homo- and hetero-polymers of guanosine-citydine (G.C) sequences were investigated using spectrophotometric and circular dichroic techniques. At pH 3.40, 10 mM [Na(+)] and 10 degrees C both polynucleotides adopted a unique and stable structural conformation different from their respective B-form structures. The protonated hetero-polymer is established as left-handed structure with Hoogsteen base pairing (H(L)-form) while the homo-polymer favored Watson-Crick base pairing with different stacking arrangements from that of B-form structure as evident from thermal melting and circular dichroic studies. The interaction of berberine, a naturally occurring protoberberine group of plant alkaloid, with the protonated structures was studied using various biophysical techniques. Binding of berberine to the H(L)-form structure resulted in intrinsic circular dichroic changes and generation of extrinsic circular dichroic bands with opposite sign and magnitude compared to its B-form structure while with the homo-polymer of G.C no such reversal of extrinsic circular dichroic bands was seen indicating different stacking arrangement of berberine at the interaction site. Scatchard analysis of the binding data, however, indicated non-cooperative binding to both the protonated forms similar to that of their respective B-form structure. Fluorescence spectral studies, on the other hand, showed remarkable increase in the intrinsic fluorescence of the alkaloid in presence of the protonated forms compared to their respective B-form structure. These results suggest that berberine could be used as a probe to detect the alteration of structural handedness due to protonation and may potentiate its use in regulatory roles for biological functions.