Fluorescence decay studies of poly(riboadenylic acid) containing 1-N6-ethenoadenosine

The fluorescence properties of the 1-N6-etheno derivatives of poly(riboadenylic acid) (poly(rA, epsilon rA)) have been examined. The fluorescence quantum yield of poly(rA, epsilon rA) decreases with an increase in the degree of the epsilon A substitution and is much smaller than that for epsilon AMP even for low degrees of epsilon A substitution. The nearest-neighbor interactions such as epsilon-adenine-adenine and epsilon-adenine-epsilon-adenine may be responsible for this behavior. It is found that the fluorescence decay kinetics obeys a three-exponential decay law for poly(rA, epsilon rA), suggesting that there exist at least three different stacked conformational states.     

The binding of poly (rA) and poly (rU) to denatured DNA. II. Studies with natural DNAs.

We have studied the interaction of poly(rA) and poly(rU) with natural DNAs containing (dA.dT)n sequences. The results indicate that hybridization of poly(rA) to denatured DNA can be used to estimate the size and frequency of large (dA.dT)n tracts, whereas hybridization with poly(rU) does not give reliable information on these points. In 6.6 M CsCl, poly(rU) can form stable complexes with denatured DNA containing short (dA)n tracts (n less than or equal to 6), whereas binding of poly(rA) to denatured DNA under these conditions requires much larger (dT)n tracts (estimated n greater than 13). Moreover, binding of poly(rA) requires pre-hybridization in low salt, because free poly(rA) precipitates in 6.6 M CsCl.     

The binding of poly(rA) and poly(rU) to denatured DNA. I. Model studies with homopolymers.

We have compared the properties of the poly(rA).oligo(dT) complex with those of the poly(rU).oligo(dA)n complex. Three main differences were found. First, poly(rA) and oligo(dT)n do not form a complex in concentrations of CsCl exceeding 2 M because the poly(rA) is insoluble in high salt. If the complex is made in low salt, it is destabilized if the CsCl concentration is raised. Complexes between poly(rU) and oligo(dA)n, on the other hand, can be formed in CsCl concentrations up to 6.6 M. Second, complexes between poly(rA) and oligo(dT)n are more rapidly destabilized with decreasing chain length than complexes between poly(rU) and oligo(dA)n. Third, the density of the complex between poly(rA) and poly(dT) in CsCl is slightly lower than that of poly(dT), whereas the density of the complex between poly(rU) and poly(dA) in CsCl is at least 300 g/cm3 higher than that of poly(dA). These results explain why denatured natural DNAs that bind poly(rU) in a CsCl gradient usually do not bind poly(rA).     

Vibrational CD study of the thermal denaturation of poly(rA) · poly(rU)

The vibrational cd (VCD) of a double-stranded RNA, poly(rA) - poly(rU), at pH 7 and moderate added salt concentration (0.1M) has been measured in both the base-stretching and phosphate-stretching regions of the ir as a function of temperature. The data in both cases show two distinct phase transitions. The first is from double- to a triple-stranded form, and the second is from triple- to single-stranded forms, which still retain substantial local order even up to 80°C. The nature of these transitions has been identified by comparison of the VCD and ir absorption spectra of the initially double-stranded samples with those of single-stranded poly(rA) and poly(rU) and with triple-stranded poly-(rA) -poly-(rU) poly (rU). The large differences in the VCD band shapes allows positive identification of the intermediate and final states. Thus under VCD-concentration conditions, a simple helix-to-coil transition can be eliminated for poly (rA ) - poly (rU) while such a two-step transition can be seen at low salt conditions. All of these observations are consistent with previous studies of the phase transitions of poly (rA) - poly (rU) under various salt conditions. Additionally, the VCD is indicative of premelting for all the triple-, double-, and single-strand complexes studied. The triple-strand complex did not show disproportionation to double strand on heating under these added salt conditions. The unusual VCD pattern for low temperature poly (rA) - poly (rU), as compared to high G? C content RNAs and DNAs, is qualitatively, but not quantitatively, explained using exciton coupling of localized dipolar transitions in each type of base within the strand. © 1993 John Wiley & Sons, Inc.     

Phase equilibrium in poly(rA).poly(rU) complexes with Cd2+ and Mg2+ ions, studied by ultraviolet, infrared, and vibrational circular dichroism spectroscopy

Ultraviolet (UV) and infrared (IR) absorption and vibrational circular dichroism (VCD) spectroscopy were used to study conformational transitions in the double-stranded poly(rA). poly(rU) and its components-single-stranded poly(rA) and poly(rU) in buffer solution (pH 6.5) with 0.1M Na+ and different Mg2+ and Cd2+ (10(-6) to 10(-2) M) concentrations. Transitions were induced by elevated temperature that changed from 10 up to 96 degrees C. IR absorption and VCD spectra in the base-stretching region were obtained for duplex, triplex, and single-stranded forms of poly(rA) . poly(rU) at [Mg2+],[Cd2+]/[P] = 0.3. For single-stranded polynucleotides, the kind of conformational transition (ordering --> disordering --> compaction, aggregation) is conditioned by the dominating type of Me2+-polymer complex that in turn depends on the ion concentration range. The phase diagram obtained for poly(rA) . poly(rU) has a triple point ([Cd2+] approximately 10(-4)M) at which the helix-coil (2 --> 1) transition is replaced with a disproportion transition 2AU --> A2U + poly(rA) (2 --> 3) and the subsequent destruction of the triple helix (3 --> 1). The 2 --> 1 transitions occur in the narrow temperature interval of 2 degrees -5 degrees . Unlike 2 --> 1 and 3 --> 1 melting, the disproportion 2 --> 3 transition is a slightly cooperative one and observed over a wide temperature range. At [Me2+] approximately 10(-3) M, the temperature interval of A2U stability is not less than 20 degrees C. In the case of Cd2+, it increases with the rise of ion concentration due to the decrease of T(m) (2-->3). The T(m) (3-->1) value is practically unchanged up to [Cd2+] approximately 10(-3)M. Differences between diagrams for Mg(2+) and Cd2+ result from the various kinds of ion binding to poly(rA).poly-(rU) and poly(rA).     

Inner-sphere complexes of divalent cations with single-stranded poly(rA) and poly(rU)

A combination of ultrasound velocimetry, density, and UV spectroscopy has been employed to study the hydration effects of binding of Mn(2+) and alkaline-earth cations to poly(rA) and poly(rU) single strands. The hydration effects, obtained from volume and compressibility measurements, are positive due to overlapping the hydration shells of interacting molecules and consequently releasing the water molecules to bulk state. The volume effects of the binding to poly(rA), calculated per mole of cations, range from 30.6 to 40.6 cm(3) mol(-1) and the compressibility effects range from 59.2 x 10(-4) to 73.6 x 10(-4) cm(3) mol(-1) bar(-1). The volume and compressibility effects for poly(rU) are approximately 17 cm(3) mol(-1) and approximately 50 x 10(-4) cm(3) mol(-1) bar(-1), respectively. The comparative analysis of the dehydration effects suggests that the divalent cations bind to the polynucleotides in inner-sphere manner. In the case of poly(rU) the dehydration effects correspond to two direct coordination, probably between adjacent phosphate groups. The optical study did not reveal any effects of cation on the secondary structure or aggregation of poly(rU). In the case of single-helical poly(rA) binding is more specific: dehydration effects correspond to three to five direct contacts and must involve atomic groups of adenines, and the divalent cations stabilize and aggregate the polynucleotide.     

An ethidium-induced double helix of poly(dA)-poly(rU).

Equilibrium dialysis, relaxation kinetic, melting, and continuous variation mixing experiments on complexes of poly(dA) and poly(rU) demonstrate that ethidium induces conversion of a 1:1 mixture of these homopolymers (at one molar salt and 19 degrees C) from a three stranded to a two stranded helix. This is the first demonstration of a double helix of poly(dA)-poly(rU) in solution.     

A fluorescence study of the binding of poly(1,N6-ethenoadenylic acid) to Escherichia coli initiation factor 3

The binding of initiation Factor 3 (IF3) to poly (1,N6-ethenoadenylic acid) [poly(epsilon A)] was investigated by fluorescence spectroscopy. At low salt concentrations, IF3 evokes an increase in the fluorescence intensity of poly(epsilon A) due to the unstacking of the nucleotide bases. The poly(epsilon A) fluorescence enhancement titrates to an endpoint of 13 +/- 2 nucleotide residues per IF3. The maximum poly(epsilon A) fluorescence enhancement, at lattice saturation, decreases with increasing salt concentration. Even though IF3 does not produce a large fluorescence increase between 75 and 200 mM NaCl concentration, the protein still binds to poly(epsilon A) at these salt concentrations as measured by sedimentation partition chromatography; the value of Kobs for the IF3-poly(epsilon A) interaction is comparable to that of other synthetic polynucleotides. The binding of IF3 to poly(A) at 150 and 200 mM NaCl induces an increase in nucleotide base-base separation as determined by CD, yet IF3-induced disruption of base stacking of poly(epsilon A) at these same salt concentrations is not detected by fluorescence. It is likely that IF3 binds primarily to the phosphate backbone of poly(epsilon A) at low salt concentrations, producing an increase in the fluorescence intensity. But, at higher salt concentrations, the aromatic amino acids intercalate between the nucleotide bases quenching the poly(epsilon A) fluorescence.     

Mg2+-induced triplex formation of an equimolar mixture of poly(rA) and poly(rU)

Magnesium ions strongly influence the structure and biochemical activity of RNA. The interaction of Mg²⁺ with an equimolar mixture of poly(rA) and poly(rU) has been investigated by UV spectroscopy, isothermal titration calorimetry, ultrasound velocimetry and densimetry. Measurements in dilute aqueous solutions at 20°C revealed two differ ent processes: (i) Mg²⁺ binding to unfolded poly(rA)·poly(rU) up to [Mg²⁺]/[phosphate] = 0.25; and (ii) poly(rA)·2poly(rU) triplex formation at [Mg²⁺]/[phosphate] between 0.25 and 0.5. The enthalpies of these two different processes are favorable and similar to each other, ~–1.6 kcal mol^–1 of base pairs. Volume and compressibility effects of the first process are positive, 8 cm³ mol^–1 and 24 × 10^–4 cm³ mol^–1 bar^–1, respectively, and correspond to the release of water molecules from the hydration shells of Mg²⁺ and the polynucleotides. The triplex formation is also accompanied by a positive change in compressibility, 14 × 10^–4 cm³ mol^–1 bar^–1, but only a small change in volume, 1 cm³ mol^–1. A phase diagram has been constructed from the melting experiments of poly(rA)·poly(rU) at a constant K⁺ concentration, 140 mM, and various amounts of Mg²⁺. Three discrete regions were observed, corresponding to single-, double- and triple-stranded complexes. The phase boundary corresponding to the transition between double and triple helical conformations lies near physiological salt concentrations and temperature.     

Poly(rA).poly(rU) with Ni(2+) ions at different temperatures: infrared absorption and vibrational circular dichroism spectroscopy

Phase transitions were studied of the sodium salt of poly(rA).poly(rU) induced by elevated temperature without Ni(2+) and with Ni(2+) in 0.07 M concentration in D(2)O (approximately 0.4 [Ni]/[P]). The temperature was varied from 20 degrees C to 90 degrees C. The double-stranded conformation of poly(rA).poly(rU) was observed at room temperature (20 degrees C-23 degrees C) with and without Ni(2+) ions. In the absence of Ni(2+) ions, partial double- to triple-strand transition of poly(rA).poly(rU) occurred at 58 degrees C, whereas only single- stranded molecules existed at 70 degrees C. While poly(rU) did not display significant helical structure, poly(rA) still maintained some helicity at this temperature. Ni(2+) ions significantly stabilized the triple-helical structure. The temperature range of the stable triple-helix was between 45 degrees C and 70 degrees C with maximum stability around 53 degrees C. Triple- to single-stranded transition of poly(rA).poly(rU) occurred around 72 degrees C with loss of base stacking in single-stranded molecules. Stacked or aggregated structures of poly(rA) formed around 86 degrees C. Hysteresis took place in the presence of Ni(2+) during the reverse transition from the triple-stranded to the double-stranded form upon cooling. Reverse Hoogsteen type of hydrogen-bonding of the third strand in the triplex was suggested to be the most probable model for the triple-helical structure. VCD spectroscopy demonstrated significant advantages over infrared absorption or the related electronic CD spectroscopy.     

The vibrational spectra and structure of poly(rA-rU)-poly(rA-rU)

Infrared and Raman spectra of aqueous poly(rA-rU)·poly(rA-rU), the double-helical complex containing strands of alternating riboadenylate and ribouridylate residues, display significant differences from one another and from corresponding spectra of poly(rA)·poly(rU), the double-helical complex of riboadenylate and ribouridylate homopolymers. Parallel studies on the copolymer and homopolymer complexes by cesium sulfate density gradient centrifugation, ultraviolet absorption spectroscopy, hydrogenion titration, 1-N oxidation of adenine residues by monoperphthalic acid and X-ray diffraction reveal, however, that the geometry of base pairing between adenine and uracil is closely similar in each complex and apparently of the Watson-Crick type. Therefore the differences observed between vibrational spectra of poly (rA-rU)·poly (rA-rU) and poly(rA)·poly(rU) are not due to different base-pairing schemes but may be attributed to differences in vibrational coupling between vertically stacked bases. Vibrational coupling may also account for the differences between infrared and Raman spectra of the same complex. Thus, the present results indicate that infrared and Raman frequencies of RNA in the region 1750–1550 cm^?1 should be dependent on the base sequence.     

Lattice vibrational modes of poly(rU)-poly(rA). A coupled single-helical approach

The eigenvalues and eigenvectors of 11-fold double-helical poly(rU)·poly(rA) have been calculated. The vibrational potential energy of the double-helical structure is initially considered to be a sum of the vibrational potential energy of the single-helical structures poly(rU) and poly(rA). Coupling between the single helices is introduced by including a stretch force constant for each hydrogen bond between the uracil and adenine base residues. In addition, a model is presented for nonbonded interactions between nearest neighbor base pairs, which is consistent with a previous model for such interactions in the single helices. Because of the simple structural relationship between the uncoupled single helices and the double helix we are able to cast the secular equation for poly(rU)·poly(rA) in a form suitable for the use of perturbation theory using the previously calculated normal modes for the single helices as the unperturbed modes. Perturbation theory was found to be inapplicable for the region of the spectrum ?450 cm^?1. In this region an exact Green function technique is used to calculate the strongly coupled modes. We explicitly display one aspect of these double-helical normal modes. The stretching motions of the hydrogen bonds in the region of the spectrum <450 cm^?1 have been plotted as bar graphs for each mode.     

Melting studies on spin-labeled polyadenylic–polyuridylic complexes

Temperature-dependent conformational transitions of spin-labeled poly rA, spin-labeled poly rU and the two-stranded helical complexes consisting either of spin-labeled rA·poly rU or spin-labeled poly rU·poly rA have been measured by electron spin resonance spectrocopy. The polynucleotides were spin labeled with 4-(2-iodoacetamido)2,2,6,6-tetramethylpiperidinooxyl and the spin label to nucleotide base ratio was approximately 1:600. The relationship between the log of tumbling time τ and the reciprocal absolute temperature for the spin-labeled single and double-stranded polynucleotides is presented. An agreement between T_m^OD (optical density melting) and T_m^sp (spin melting) is found for the complexes, which strongly supports the conclusion that the same temperature-dependent structural changes are monitored with both techniques.     

The poly dA strand of poly dA.poly dT adopts an A-form in solution: a UV resonance Raman study.

The study by resonance Raman spectroscopy with a 257 nm excitation wave-length of adenine in two single-stranded polynucleotides, poly rA and poly dA, and in three double-stranded polynucleotides, poly dA.poly dT, poly(dA-dT).poly(dA-dT) and poly rA.poly rU, allows one to characterize the A-genus conformation of polynucleotides containing adenine and thymine bases. The characteristic spectrum of the A-form of the adenine strand is observed, except small differences, for poly rA, poly rA.poly rU and poly dA.poly dT. Our results prove that it is the adenine strand which adopts the A-family conformation in poly dA.poly dT.     

Interaction of quinacrine mustard with mononucleotides and polynucleotides

1. The interaction between quinacrine mustard and mononucleotides and polynucleotides was investigated by fluorimetry and absorbance spectrophotometry. 2. The fluorescence spectrum of quinacrine mustard is independent of the ionic strength and pH. The dependence of the quinacrine mustard fluorescence intensity on ionic strength, pH and anions is described. 3. The fluorescence intensity of quinacrine mustard was enhanced with the mononucleotide adenylic acid and polynucleotides such as poly(rA), poly(rU) and poly(rA,rU). 4. Quenching of the fluorescence intensity of quinacrine mustard occurred with the mononucleotide guanylic acid and with poly(rG) and poly(rC,rG). 5. The mononucleotide cytidylic acid or poly(rC) showed no effect on the fluorescence intensity of quinacrine mustard. 6. The interaction between the dye and native DNA species was also dependent on the presence of base-specific binding sites in the DNA. The higher the (G+C) content was in the native DNA tested the higher was the quenching effect on the fluorescence intensity of quinacrine mustard. 7. No interaction was found between the dye and methylated DNA. The binding between quinacrine mustard and apurinic DNA was confirmed to be in the phosphate groups of the purines.     

Gel electrophoretic analysis of poly(riboadenylic acid)

It is shown that molecular weights and molecular-weight distributions of poly(rA), and by implication other single-stranded polynucleotides, and synthetic and natural polyelectrolytes in general, can be determined by electrophoresis in polyacrylamide gels. It is shown that fractions of very narrow molecular-weight distribution can be obtained by preparative electrophoresis of polydisperse samples. Molecular-weight calibrations based on sedimentation coefficients of such fractions are given, and in aqueous systems do not coincide with calibrations for partially base-paired RNA species. Poly(rU) fractions fall on the same calibration as poly(rA). Relations between mobilities, relative to standard markers, and molecular weight for poly(rA) over a wide range of molecular weights are given, which allow rapid molecular-weight determination on poly(rA) samples, such as the segments found in many types of messenger RNA.     

Triple helical polynucleotidic structures: sugar conformations determined by FTIR spectroscopy.

Fourier Transform Infrared Spectra of triple stranded polynucleotides containing homopurine dA or rA and homopyrimidine dT or rU strands have been obtained in H2O and D2O solutions as well as in hydrated films at various relative humidities. The spectra are interpreted by comparison with those of double stranded helixes with identical base and sugar composition. The study of the spectral domain corresponding to in-plane double bond stretching vibrations of the bases shows that whatever the initial duplex characterized by a different IR spectrum (A family form poly rA.poly rU, heternomous form poly rA.poly dT, B family form poly dA.poly dT), the triplexes present a similar IR spectrum reflecting similar base interactions. A particular attention is devoted to the 950-800 cm-1 region which contains marker bands of the sugar conformation in the nucleic acids. In solution the existence of only N (C3'endo-A family form) type of sugar pucker is detected in poly rU.poly rA.poly rU and poly dt.poly rA.poly rU. On the contrary absorption bands characteristic of both N (C3'endo-A family form) and S (C2'endo-B family form) type sugars are detected for poly rU.poly rA.poly dT, poly rU.poly dA.poly dT and poly dT.poly rA.poly dT. Finally mainly S (C2'endo-B family form) type sugars are observed in poly dT.poly dA.poly dT.     

Induced circular dichroism in nucleic acid-acridine derivative complexes

Visible absorption and circular dichroism (CD) spectra have been measured for complexes formed between nucleic acids (calf thymus DNA, poly(rA).poly(rU) and poly(rI).poly(rC)) and 9-aminoacridines (quinacrine, acranil and 9-amino-6-chloro-2-methoxy acridine). With poly(rA).poly(rU), a new absorption band was observed at longer wavelengths. The nucleic acid-drug complexes showed considerable different induced CD spectra. Analysis of these CD spectra suggests that the cationic side chains of quinacrine and acranil play an important role on the binding properties to DNA and poly(rA).poly(rU).     

Studies on spin-labeled polyriboadenylic acid

Spin-labeled samples of poly rA, poly rU, and poly rG have been prepared, and physicochemical properties primarily of labeled poly rA are reported. The nitroxide radical, 4-(2-iodoacetamido)-2,2,6,6-tetramethylpiperidinooxyl, is incorporated to a greater extent in poly rA and poly rU, as compared to poly rG. No incorporation is observed in the case of poly rC. Special attention has been paid to the separation of the covalently attached labels from the free labels, and to the preservation of the integrity of the chain length of the labeled polymers. The determination of molar extinction coefficients of the three labeled polymers indicates virtually no difference from those known for the chemically unpertubed polyribonucleotides. The correlation times for the spin-labeled single stranded poly rA and poly rU have been calculated. More mobile building blocks are found in poly rU as compared to poly rA. Conformational properties of labeled poly rA in aqueous solutions have been investigated using electron spin resonance, circular dichroism, and absorption spectroscopy. The objective of the study of labeled poly rA was to examine its conformational transitions upon the uptake of protons by the adenine bases. Based on electron spin resonance data there is strong evidence that the single strand-double strand transition can take place in three steps. In addition to the already known two forms of double-stranded poly rA in acidic solution, called A and B, it is suggested that a third phase, consisting possibly of large aggregates, is involved in the transition of the less protonated double strands to those of complete protonation.     

Raman spectral studies of nucleic acids. XVII. Conformational structures of polyinosinic acid.

Laser-Raman spectra of poly(rI) show the formation of an ordered complex in aqueous solutions of high ionic strength. This structure exhibits the A-helix geometry, contains stacked bases and is apparently stabilized by specific hydrogen bonding involving hypoxanthine C6=0 groups. Thermal dissociation of the poly(rI) complex (Tm=45 degrees C) yields single-stranded and disordered poly (RI) chains. A disordered structure also occurs for poly (rI) in aqueous solutions of low ionic strength. In oriented films, poly (rI) forms an ordered structure probably the same as that which occurs in solutions of high ionic strength. Raman intensities measured at 815 and 1100 cm-1 in spectra of poly (rI) and poly (rU)-poly (rA)-poly(rU) indicate that the correlation previously established for single- and double-stranded ribopolymer structures is valid also for these multi-stranded structures. X-ray diffraction and model-building studies confirm the A-helix structure.