Cooperative disordering of single-stranded polynucleotides through copper crosslinking

The thermal transitions of single-stranded polynucleotides are noncooperative. In contrast, Cu(II) cooperatively disorders the single-stranded helical structures of poly(A) and poly(C), as demonstrated by ORD and UV spectral changes as a function of the Cu²⁺ activity, and by a dramatic chain-length dependence of the spectral changes. Equilibrium dialysis binding studies indicate that the cooperative disordering is paralleled by a somewhat less cooperative binding process. The difference between the thermal- and Cu(II)-induced transition is explained by the following mechanism. (1) Cu(II) initially binds in a noncooperative fashion to phosphate. (2) The Cu(II) so bound forms a second bond to a nonadjacent base site on the same polymer strand or another strand. These intramolecular and intermolecular crosslinks to the bases are responsible for the disordering. (3) The initial crosslinks formed provide nuclei for the cooperative formation of additional crosslinks, producing cooperative spectral changes paralleled by cooperative binding. A comparison of the spectral and binding transitions indicates that there is appreciable noncooperative binding of copper to phosphate, which produces no spectral changes in the presence of added electrolyte. This comparison also indicates that each copper crosslink disorders several bases. The formation of intermolecular crosslinks is demonstrated by a polymer concentration dependence of the disordering. The formation of intramolecular crosslinks can be deduced from the fact that the “cooperative unit” required to explain the differences between the hexamer, which does not readily form intramolecular crosslinks, and the polymer is considerably larger than the cooperative unit determined from the polymer results. The poly(A) disordering transition is less symmetrical than that of poly(C), particularly at low polymer concentrations. These results, together with other phenomena, are explained by a greater flexibility of poly(A), which favors the formation of small intramolecular loops.     

Dissociation of double-stranded poly(I) . poly(C) by cis-diammine-dichloro-Pt(II).

The covalent binding of cis-Pt(NH3)2Cl2 on the double stranded poly(I) . poly(C) induced an irreversible dissociation of the two strands. This dissociation was evidenced mainly by poly(I)-Agarose affinity chromatography which allowed to recover free strands of cis-Pt(NH3)2Cl2-poly(I) from a cis-Pt(NH3)2Cl2-poly(I) . poly(C) complex, by density equilibrium centrifugation where free poly(C) could be isolated, and by acid titrations of the metal-poly(I) . poly(C) complexes. The separation of the two strands of the polyribonucleotide upon cis-Pt(NH3)2Cl2 fixation was shown not to exceed 90--95%. A dissociation curve of the polynucleotide double helix as a function of the amount of bound cis-Pt(NH3)2Cl2 was determined and was shown to be of a characteristic cooperative effect. The fixation of the paltinum compound to poly(I) . poly(C) seemed also to be cooperative.     

Nanopore detachment kinetics of poly(A) binding proteins from RNA molecules reveals the critical role of C-terminus interactions

The ubiquitous and abundant cytoplasmic poly(A) binding protein (PABP) is a highly conserved multifunctional protein, many copies of which bind to the poly(A) tail of eukaryotic mRNAs to promote translation initiation. The N-terminus of PABP is responsible for the high binding specificity and affinity to poly(A), whereas the C-terminus is known to stimulate PABP multimerization on poly(A). Here, we use single-molecule nanopore force spectroscopy to directly measure interactions between poly(A) and PABPs. Both electrical and biochemical results show that the C-C domain interaction between two consecutive PABPs promotes cooperative binding. Up to now, investigators have not been able to probe the detailed polarity configuration (i.e., the internal arrangement of two PABPs on a poly(A) streak in which the C-termini face toward or away from each other). Our nanopore force spectroscopy system is able to distinguish the cooperative binding conformation from the noncooperative one. The ～50% cooperative binding conformation of wild-type PABPs indicates that the C-C domain interaction doubles the cooperative binding probability. Moreover, the longer dissociation time of a cooperatively bound poly(A)/PABP complex as compared with a noncooperatively bound one indicates that the cooperative mode is the most stable conformation for PABPs binding onto the poly(A). However, ～50% of the poly(A)/PABP complexes exhibit a noncooperative binding conformation, which is in line with previous studies showing that the PABP C-terminal domain also interacts with additional protein cofactors.     

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.     

Structural transitions in polyadenylic acid and hypothesis on biological role of its double-stranded forms

Under various conditions poly(A) exists in different forms such as single-stranded helix, two double-helical forms and others. The formation of double-stranded helices is induced by adenine protonation. Under physiological ionic strengths they are formed at acidic pH, but under the same conditions methylated poly(A) has double-stranded structure at alkaline pH. Since the shift of adenine protonation pKa to alkaline region may be caused not only by chemical modification of poly(A) but also its interaction with proteins, it is quite probable that double oligo(A)-helices are formed in the living cell as well. In this article the hypothesis on possible biological role of poly(A) double-stranded forms has been discussed in details. The models of involvement of double oligo(A)-sequences of RNA in such intracellular processes as termination of mRNA poly(A) tails synthesis and autoregulation of poly(A)-binding protein synthesis are suggested as an example.     

Escherichia coli single-stranded DNA binding protein is mobile on DNA: 1H NMR study of its interaction with oligo- and polynucleotides

The interaction of the Escherichia coli single-stranded DNA binding protein (SSB) with oligo- and poly-nucleotides has been studied by 270-MHz 1H NMR spectroscopy and fast kinetic techniques. d(pT)8 and poly(dT) were used to study noncooperative and cooperative binding, respectively. The H6, H1', and CH3 resonances of d(pT)8 are high-field shifted by less than 0.05 ppm, and H8 and H2 of poly(dA) are low-field shifted upon complexation. The protein resonances remain virtually unshifted. The small shifts upon complexation provide no evidence for extensive stacking interactions between the nucleotide bases and aromatic amino acid side chains of SSB. The d(pT)8 and poly(dA) signals are broadened to about 30 Hz whereas the resonances of poly(dT) are broadened beyond detection upon stoichiometric complexation. Continuous broadening of all poly(dT) signals even at a 10-fold excess of poly(dT) indicates fast exchange of SSB between different binding sites. Dissociation and reassociation rates determined from stopped-flow experiments are too slow by at least 2 orders of magnitude to account for the experimental line widths. Therefore, we conclude that SSB translocates without dissociation from the DNA template. A model for the translocation is outlined. It is based on partial dissociation of octamer sections of poly(dT) from the complex with a rate constant as previously published for the dissociation of d(pT)8 from SSB.     

Open states in native polynucleotides. II. Hydrogen-exchange study of cytosine-containing double helices.

Hydrogen-exchange studies of I · C and G · C double helices were carried out to test the generality of conclusions reached previously in studies of adenine-containing polymers (preceding paper). The cytosine amino group shows hydrogen-exchange behavior similar to the analogous group in adenine; a pH-independent pathway and a parallel general catalysis pathway require prior separation of the base-pair and pre-equilibrium protonation at the ring N. The cytosine amino group does, however, display greater sensitivity to specific and to general catalysis than found for adenine. In the G · C helix, the ring NH proton of guanine exchanges at the opening-limited rate, as does the analogous proton in A · U and A · T pairs, while the guanine amino protons exchange without a prior opening of structure. From the observed exchange rates and the known chemistry for the pH-independent reaction, one can calculate equilibrium opening constants of 4 × 10⁻³ for poly(rI) · poly(rC) and perhaps one tenth of that for poly(rG) · poly(rC). Also the opening rate constant for the G · C helix is 0.01 s⁻¹.These results, when applied to published exchange curves for DNA, indicate an equilibrium opening constant of 0.005, an opening rate constant of 0.04 s⁻¹, and a closing rate constant of 10 s⁻¹. (All values refer to studies at 0 °C.) These values point to the same kind of traveling-loop model for base-pair opening discussed previously for the opening reactions in adenine-containing double helices.     

Effect of DEAE-dextran upon the interaction of polynucleotides in poly (l+c) double complex]

It has been shown that the formation of poly(I+C) double complex is accompanied by appearance of the 244 nm CD band which is absent from the spectrum of the initial components. The amplitude of this CD band is maximum upon equimolar ratio of components. When one mixes the complementary polynucleotides bound to DEAE-dextran (D-d) double comples is not formed. CD spectrum of poly (I+C) double complex is changed considerably upon addition of D-d: CD increases when P/N ratio is 10:1, decreases at P/N 1:1 and comes back to the initial spectrum at P/N 1:5. Thermal dissociation of poly(I+C) when the anionic component was in surplus was similar to poly(I+C) alone (Tm equals 67 degrees) when the polydextran was in excess; the thermal dissociation was lower (Tm equals 43 degrees) than that of poly (I+C). It is discussed the possible mechanism of the D-d and poly (I+C) interaction.     

Structural and conformational studies of polyriboadenylic acid in neutral and acid solution

Raman spectra of solutions of polyriboadenylic acid have been studied in the pH range of 7.2–5.2. Bands are identified which are sensitive to the characteristics of poly(rA) in the single-and double-stranded helical forms. Thermal melting profiles were obtained as a function of pH to monitor simultaneously the changes in (1) the phosphodiester backbone, (2) the base-stacking interactions, (3) the perturbation of the PO unit, and (4) the degree of protonation at the N-1 position in the adenine base. The temperature dependence of the intensity ratio of the bands at 725 and 705 cm^?1 appears to be sensitive to the noncooperative and the cooperative thermal-melting process for the single-and double-stranded forms of poly(rA), respectively. Concurrently, bands diagnostic of the degree of protonation reveal that the cooperative melting process for the “acid” poly(rA) clearly involves deprotonation. The progressive perturbation of the 1100 cm^?1 band with an increasing degree of protonation of poly(rA) is consistent with earlier suggestions regarding a PO-(6)-NH₂ interaction in the double-helical form of poly(rA). The stability of the double-helix parallels the degree of protonation over the pH range studied as reflected in the t_m values, which increase linearly with decreasing pH.     

Crystal structure of a poly(rA) staggered zipper at acidic pH: evidence that adenine N1 protonation mediates parallel double helix formation

We have solved at 1.07 Å resolution the X-ray crystal structure of a polyriboadenylic acid (poly(rA)) parallel and continuous double helix. Fifty-nine years ago, double helices of poly(rA) were first proposed to form at acidic pH. Here, we show that 7-mer oligo(rA), i.e. rA₇, hybridizes and overlaps in all registers at pH 3.5 to form stacked double helices that span the crystal. Under these conditions, rA₇ forms well-ordered crystals, whereas rA₆ forms fragile crystalline-like structures, and rA₅, rA₈ and rA₁₁ fail to crystallize. Our findings support studies from ∼50 years ago: one showed using spectroscopic methods that duplex formation at pH 4.5 largely starts with rA₇ and begins to plateau with rA₈; another proposed a so-called ‘staggered zipper’ model in which oligo(rA) strands overlap in multiple registers to extend the helical duplex. While never shown, protonation of adenines at position N1 has been hypothesized to be critical for helix formation. Bond angles in our structure suggest that N1 is protonated on the adenines of every other rAMP−rAMP helix base pair. Our data offer new insights into poly(rA) duplex formation that may be useful in developing a pH sensor.     

Study of the interaction of cis-dichloro-(1,2 diethyl-3-aminopyrrolidine)Pt(II) complex with poly(I), poly(C) and poly(I) x poly(C)

The interaction of cis-dichloro-(1,2 diethyl-3-aminopyrrolidine)platinum(II) (Ptpyrr) with the polynucleotides poly(I), poly(C) and poly(I) x poly(C) acids was studied by circular dichroism, molecular fluorescence and (1)H NMR spectroscopies. Multivariate Curve Resolution, a factor analysis method, was applied for the analysis and interpretation of spectroscopic data obtained in mole ratio and kinetics studies. This procedure allows the determination of the number of different interaction complexes present during the experiments and the resolution of both concentration profiles and pure spectra for all of them. Two different interaction complexes were observed at the experimental conditions studied. The first one, at low Ptpyrr:polynucleotide ratio (r(Ptpyrr:poly)) values, corresponds to the interaction of Ptpyrr with hypoxanthine bases in the poly(I) moiety. This interaction leads to the destabilization and dissociation of the double-stranded conformation. The second complex was observed at higher r(Ptpyrr:poly) values and corresponds to the interaction of Ptpyrr to cytosine bases in poly(C) moiety. The formation of both complexes showed that the interaction of Ptpyrr with hypoxanthine bases occurred at the first stages of the reaction and with cytosine bases at longer reaction times. The results obtained show the utility of the Multivariate Curve Resolution approach for the analysis of data obtained by monitoring spectroscopically the interaction equilibria of platinum compounds with nucleic acids.     

Polynucleotides. LVI. Synthesis and properties of poly(2-deoxy-2''-fluoroinosinic acid).

Poly (2'-deoxy-2'-fluoroinosinic acid) [ poly(If)] was synthesized by polymerization of 2'-deoxy-2'-fluoroinosine 5'-diphosphate catalyzed by Escherichia coli polynucleotide phosphorylase. Although the UV absorption properties of poly(If) closely resembled those of poly(I), thermal melting curves at Na+ concentrations of 0.15M and 0.75M suggested two ordered structures for poly(If) neutral form. CD psectra taken at 0.15M Na+ concentration showed rather larger amplitudes in both a peak at 273 nm and a trough at 246 nm, suggesting rather strong vertical stacking of bases. When complexed with poly(C), poly(If) forms a double-stranded complex, poly(If).poly(C) which has Tm's higher by 10-20 degrees than those of poly(If).poly(C) measured under the same conditions. The CD spectrum of this complex resembled that of poly(I).poly(C). The effect of the fluorine atom at the 2'-position on thermal stability of polynucleotides is discussed.     

Excluded-volume effect of inert macromolecules on the melting of nucleic acids

It is shown on the basis of the excluded-volume effect that inert macromolecules may be expected to suppress the dissociation of double-helical nucleic acids into single helices and thus to raise the melting point of the double helix. The rise in melting temperature of the ribonucleic acid [poly(I).poly(C)] caused by dextran polymers and by poly(ethylene oxide) is described and compared with the theoretical prediction. Good agreement was found in respect of the extent of the rise in melting point and in respect of its dependence upon polymer length. An additional dependence upon the identify of the polymer was attributed to detailed effects of shape in solution.     

Structure of the hydration shells of oligo(dA-dT).oligo(dA-dT) and oligo(dA).oligo(dT) tracts in B-type conformation on the basis of Monte Carlo calculations

Monte Carlo simulations [(N, V, T)-ensemble] were performed for the hydration shell of poly(dA-dT).poly(dA-dT) in canonical B form and for the hydration shell of poly(dA).poly(dT) in canonical B conformation and in a conformation with narrow minor groove, highly inclined bases, but with a nearly zero-inclined base pair plane (B' conformation). We introduced helical periodic boundary conditions with a rather small unit cell and a limited number of water molecules to reduce the dimensionality of the configuration space. The coordinates of local maxima of water density and the properties of one- and two-membered water bridges between polar groups of the DNA were obtained. The AT-alternating duplex hydration mirrors the dyad symmetry of polar group distribution. At the dApdT step, a water bridge between the two carbonyl oxygens O2 of thymines is formed as in the central base-pair step of Dickerson's dodecamer. In the major groove, 5-membered water chains along the tetranucleotide pattern d(TATA).d(TATA) are observed. The hydration geometry of poly(dA).poly(dT) in canonical B conformation is distinguished by autonomous primary hydration of the base-pair edges in both grooves. When this polymer adopts a conformation with highly inclined bases and narrow minor groove, the water density distribution in the minor groove is in excellent agreement with Dickerson's spine model. One local maximum per base pair of the first layer is located near the dyad axis between adjacent base pairs, and one local maximum per base pair in the second shell lies near the dyad axis of the base pair itself. The water bridge between the two strands formed within the first layer was observed with high probability. But the water molecules of the second layer do not have a statistically favored orientation necessary for bridging first layer waters. In the major groove, the hydration geometry of the (A.T) base-pair edge resembles the main features of the AT-pair hydration derived from other sequences for the canonical B form. The preference of the B' conformation for oligo(dA).oligo(dT) tracts may express the tendency to common hydration of base-pair edges of successive base pairs in the grooves of B-type DNA. The mean potential energy of hydration of canonical B-DNA was estimated to be -60 to -80 kJ/mole nucleotides in dependence on the (G.C) contents. Because of the small system size, this estimation is preliminary.     

Studies of bivalent copper ion binding to poly C

Ultraviolet differential spectra of single-stranded poly C, taken in the presence of Cu2+ ions, are studied at various ionic strengths and temperatures. Coordinational and conformational components of these spectra are obtained. The Cu2+ ion coordination site on the polynucleotide bases is found to be N(3) and possibly O(2). The direction of the poly C absorption band shift due to ion binding and conformational transitions is established. At low ionic strengths of the solution Cu2+ ions cause the helical parts of poly C to melt. At high ones the formation of double-stranded parts was observed in addition to the above effect. The calculated concentration dependences of ion-poly C bases association constants show that binding is cooperative at any ionic strength.     

Buffer catalysis of amino proton exchange in compounds of adenosine, cytidine and their endocyclic N-methylated derivatives

The use of buffer catalysts having a wide range of pK (dissociation) values (4-12) provides the first estimates of two generally useful empirical parameters of amino proton exchange in compounds of adenine and cytosine. These are a nucleobase amino group dissociation constant (pKD) and the 'encounter frequency' for proton transfer (kD), which can be used to predict amino proton exchange rates. Values of amino pKD fall in the range 8.6-9.4 for the unsubstituted nucleobases and their endocyclic N-methylated derivatives. Similar values of kD are obtained for all nucleobases (1 X 10(8) M-1 s-1). These constants were obtained from a statistical fit of second-order catalytic rate constants for amino proton exchange, measured by amino 1H-NMR lineshape at varying field frequencies (100, 300 and 360 MHz). These results confirm the requirement for buffer conjugate base formation and nucleobase protonation, but point to a different mechanism of exchange at low pH; most probably direct amino protonation for adenine, but not for cytosine compounds. Anionic buffer conjugate bases (phosphate and acetate) show a greater catalytic effect than neutral (nitrogen) bases, especially with cytosine compounds. The use of high concentrations of sodium perchlorate to sharpen amino 1H resonances of 1-methyladenosine is examined, with respect to chemical and rotational exchange and NMR line broadening.     

DNA triple helix stabilization by aminoglycoside antibiotics

The stabilization of the poly(dA) x 2poly(dT) triple helix by neomycin is reported. Preliminary results indicate that neomycin stabilizes DNA triple helices and the double helical structures composed of poly(dA) x poly(dT) are virtually unaffected. This is the first report of the interaction of aminoglycoside antibiotics with DNA triple helices.     

Analysis of difference spectra of protonated DNA: determination of degree of protonation of nitrogen bases and the fractions of disordered nucleotide pairs.

The titration curves of nitrogen bases and fractions of disordered nucleotide pairs are obtained during DNA protonation. It is shown that purine bases are the first sites of the DNA double helix protonation. The cytosine protonation is due to proton-induced conformational transition within GC pairs with the sequence proton transfer from (N-7) of guanine to (N-3) of cytosine. Within DNA with unwound regions the bases are protonated in the following order: cytosine, adenine, guanine. It is shown that GC pairs are the primary centres in which the unwinding of protonated DNAs occurs.     

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 structure of triple helical poly(U).poly(A).poly(U) studied by Raman spectroscopy

Using Raman spectroscopy, we examined the ribose-phosphate backbone conformation, the hydrogen bonding interactions, and the stacking of the bases of the poly(U).poly(A).poly(U) triple helix. We compared the Raman spectra of poly(U).poly(A).poly(U) in H2O and D2O with those obtained for single-stranded poly(A) and poly(U) and for double-stranded poly(A).poly(U). The presence of a Raman band at 863 cm-1 indicated that the backbone conformations of the two poly(U) chains are different in the triple helix. The sugar conformation of the poly(U) chain held to the poly(A) by Watson-Crick base pairing is C3' endo; that of the second poly(U) chain may be C2' endo. Raman hypochromism of the bands associated with base vibrations demonstrated that uracil residues stack to the same extent in double helical poly(A).poly(U) and in the triple-stranded structure. An increase in the Raman hypochromism of the bands associated with adenine bases indicated that the stacking of adenine residues is greater in the triple helix than in the double helical form. Our data further suggest that the environment of the carbonyls of the uracil residues is different for the different strands.