Raman spectral studies of nucleic acids. XVI. Structures of polyribocytidylic acid in aqueous solution

Raman spectra of polyribocytidylic acid show the formation of an ordered single-stranded structure [poly(rC)] at neutral pH and an ordered double-stranded structure containing hemiprotonated bases [poly(rC)·poly(rC⁺)] in the range 5.5 > pH > 3.7. Below 40°C, poly(rC) contains stacked bases and a backbone geometry of the A-type, both of which are gradually eliminated by increasing the temperature to 90°C. Below 80°C, poly(rC)·poly(rC⁺) contains bases which are hydrogen bonded and stacked and a backbone geometry also of the A-type. In this structure the bases of each strand are shown to be structurally identical, i.e., hemiprotonated, and therefore distinct from both neutral and protonated cytosines. Infrared and Raman spectra indicate the existence of a center of symmetry with respect to the paired cytosine residues, which suggests that the additional proton per base pair is shared equally by the two hydrogen-bonded bases. Denaturation of poly(rC)·poly(rC⁺) occurs cooperatively (t_m ≈ 80°C) with elimination of base stacking, base pairing, and the A-helix geometry. Each of the separated strands of the denatured complex is shown to contain comparable amounts of both neutral and protonated cytosines, most likely in alternating sequence [poly(rC, rC⁺)]. In both poly(rC, rC⁺) and poly(rC), at 90°C, the backbones do not exhibit the phosphodiester Raman frequencies characteristic of other disordered polyribonucleotide chains. This is interpreted to mean that the single strands, though devoid of base stacking and A-type structure, contain uniformly ordered backbones of a specific type. Fully protonated poly(rC⁺), on the other hand, forms no ordered structure and may be characterized as a disordered (random chain) polynucleotide at all temperatures. Several Raman lines of poly(rC) are absent from the spectrum of poly(rC)·poly(rC⁺) and vice versa. These frequencies, assigned mainly to vibrations of the ribose groups, suggest that the furanose ring conformations are different in the single-stranded and double-stranded structures of polyribocytidylic acid. Several other Raman group frequencies have been identified and correlated with the polymer secondary structures.     

The interaction of Na ions with synthetic polynucleotides

The interaction of Na⁺ with poly A, poly U, poly A·poly U, and Poly A·2 poly U has been investigated by means of potentiometry, by means of potentiometry, by means of a linked-function analysis of its effect on the binding of Mg⁺⁺ ions, and of K⁺ by means of an analysis of its effect on the sedimentation coefficients of the polymers. The last method was found to be inapplicable. The results of the other two methods were found to be consistent, except in the case of poly A where the existence of base stacking, influenced by the binding of Mg⁺⁺, significantly affects the linked-function analysis. The results are also consistent with the effects of the concentration of Na⁺ ions on the thermally induced conformational transitions of poly A·poly U and poly A·2 poly U, and with the extents of “binding” of Na⁺ to DNA measured by equilibrium and by transport methods. The interaction of Na⁺ with polynucleotides appears to be physically quite specific, although its thermodynamic basis is not clear. The extent of binding of Na⁺, Ψ, was found to be independent of the total Na⁺ concentration but a quadratic function of the extent of Mg⁺⁺ binding, θ. In the absence of Mg⁺⁺, Ψ = 0.35–0.38 for poly U, 0.40 for poly A, 0.59 for poly A·poly U, and 0.66 for poly A·2 poly U.     

The Structure of Triple Helical Poly(U)·Poly(A)·Poly(U) Studied by Raman Spectroscopy

Abstract

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.     

A Molecular Dynamics Simulation Study of Coaxial Stacking in RNA

Abstract

We report on unrestrained molecular dynamics simulations of an RNA tetramer binding to a tetra-nucleotide overhang at the 5′-end of an RNA hairpin (nicked structure) and of the corresponding continuous hairpin with Na⁺ as counterions. The simulations lead to stable structures and in this way a structural model for the coaxially stacked RNA hairpin is generated. The stacking interface in the coaxially stacked nicked hairpin structure is characterized by a reduced twist and shift and a slightly increased propeller twist as compared to the continuous system. This leads to an increased overlap between C22 and G23 in the stacking interface of the nicked structure. In the simulations the continuous RNA hairpin has an almost straight helical axis. On the other hand, the corresponding axis for the nicked structure exhibits a marked kink of 39°. The stacking interface exhibits no increased flexibility as compared to the corresponding base pair step in the continuous structure.     

Towards a DNA-Like Duplex Without Hydrogen Bonds

Abstract

The inverse quadrupolar moments of the phenyl and pentafluorophenyl residues in the base pair P-F⁵ promotes strong intramolecular stacking interactions in DNA duplexes. The more natural base pairs are replaced by this novel pair the higher the thermodynamic stability of the resulting duplex if they are arranged in an alternating fashion.     

Theoretical studies on protein-nucleic acid interactions. II. Hydrogen bonding of amino acid side chains with bases and base pairs of nucleic acids

With a view to understanding the role of hydrogen bonds in the recognition of nucleic acids by proteins, hydrogen bonding between the bases and base pairs of nucleic acids and the amino acids (Asn, Gln, Asp and Glu, and charged residues Arg⁺, Glu^?, and Asp^?) has been studied by a second-order perturbation theory. Binding energies have been calculated for all possible configurations involving a pair of hydrogen bonds between the base (or base pair) and the amino acid residue. Our results show that the hydrogen bonding in these cases has a large contribution from electrostatic interaction. In general, the charged amino acids, compared to the uncharged ones, form more stable complexes with bases or base pairs. The hydrogen-bond energies are an order of magnitude smaller than the Coulombic interaction energies between basic amino acids (Lys⁺, Arg⁺, and His⁺) and the phosphate groups of nucleic acids. The stabilities of the complexes of amino acids Asn, Gln, Asp, and Glu with bases are in the order: G–X > C–X > A–X U–X or T–X, and G · C–X > A · T(U)–X, where X is one of these amino acid residues. It has been shown that Glu^? and Asp^? can recognize guanine in single-stranded nucleic acids; Arg⁺ can recognize G · C base pairs from A · T base pairs in double-stranded structures.     

The effect of monovalent cations on the association behavior of guanosine 5'-monophosphate, cytidine 5'-monophosphate, and their equimolar mixture in aqueous solution

¹H- and ³¹P-nmr spectroscopy have been used to investigate the self-association of M₂(5′-CMP) [M = Li⁺, Na⁺, K⁺, Rb⁺, or (CH₃)₄ N⁺; 5′-CMP = cytidine 5′-monophosphate], the self-association of Li₂(5′-GMP) (5′-GMP = guanosine 5′-monophosphate), and the heteroassociation of 5′-GMP and 5′-CMP (1 : 1 mole ratio) in aqueous solution as a function of the nature of the monovalent cation. Proton spectral differences for the different 5′-CMP salts exhibit a cation-size dependence and have been ascribed to a change in the stacking geometry. An average stacking association constant of 0.63 ± 0.24M^?1 at 1°C, consistent with the weak stacking interactions of the cytosine bases, was determined for the 5′-CMP salts. Heteroassociation of 5′-GMP and 5′-CMP follows the reverse of the cation order for the formation of ordered aggregates of 5′-GMP. Heteroassociation occurs in the presence of Li⁺, Na⁺, and Rb⁺ ions, but only self-association occurs for the K⁺ nucleotides. Li₂(5′-GMP), which does not form ordered species, self-associates to form disordered base stacks with a stacking constant of 1.63 ± 0.11M^?1 at 1°C.     

Density functional theory study of the potassium complexation of an unsymmetrical 1,3-alternate calix[4]-crown-5-N-azacrown-5 bearing two different crown rings

Theoretical studies of an unsymmetrical calix[4]-crown-5-N-azacrown-5 (1) in a fixed 1,3-alternate conformation and the complexes 1·K⁺(a), 1·K⁺(b), 1·K⁺(c) and 1·K⁺K⁺ were performed using density functional theory (DFT) at the B3LYP/6-31G* level. The fully optimized geometric structures of the free macroligand and its 1:1 and 1:2 complexes, as obtained from DFT calculations, were used to perform natural bond orbital (NBO) analysis. The two main types of driving force metal–ligand and cation–π interactions were investigated. NBO analysis indicated that the stabilization interaction energies (E ₂) for O…K⁺ and N…K⁺ are larger than the other intermolecular interactions in each complex. The significant increase in electron density in the RY* or LP* orbitals of K⁺ results in strong host–guest interactions. In addition, the intermolecular interaction thermal energies (ΔE, ΔH, ΔG) were calculated by frequency analysis at the B3LYP/6-31G* level. For all structures, the most pronounced changes in the geometric parameters upon interaction are observed in the calix[4]arene molecule. The results indicate that both the intermolecular electrostatic interactions and the cation–π interactions between the metal ion and π orbitals of the two pairs that face the inverted benzene rings play a significant role.     

Thermodynamics of base interaction in (A)n and (A.U)n

Using precision scanning microcalorimetry we studied (A)_n and (A·U)_n melting in highly diluted solutions (0.3 to 5.0 mm) with different Na⁺ activity. This permitted us to determine directly the thermodynamic functions of stacking interaction in (A)_n and base-pairing in (A·U)_n. For (A-A) stacking at (A)_n melting temperature we obtained ΔH^(A)n_m = 12.6 kJ mol^?1; ΔS^(A)n_m = 41 J K^?1 mol^?1. For A·U base-pairing at a standard temperature of 298 K and 0.1 m-Na⁺ we have: ΔH^(A·U) = 34 kJ mol^?1; ΔS^(A·U) = 102 J K^?1 mol^?1ΔG^(A·U) = ?3.5 kJ mol^?1.     

Selective Metalation of 6-Methylpurines: Synthesis of 6-Fluoromethylpurines and Related Nucleosides

Abstract

A selective metalation at the 6-CH3 over C-8 of 6-methylpurine derivative 6 was observed with softer counter cation (Na⁺ or K⁺) of the base, while the harder Li⁺ showed no selectivity. In the presence of N-fluorobenzenesulfonamide (NFSI), this property was utilized for the synthesis of 6-fluoromethylpurine derivatives 4 and 5 as potential toxins for suicide gene therapy.     

Macrocyclic zinc(II) complexes for selective recognition of nucleobases in single- and double-stranded polynucleotides

 As an extension of our earlier discoveries that Zn^II-cyclen complex (1) (cyclen=1,4,7,10-tetraazacyclododecane) and Zn^II-acridine-pendant cyclen complex Zn^II-N-(9-acridin)ylmethyl-cyclen (3) are the first compounds to selectively recognize thymidine and uridine nucleosides in aqueous solution at physiological pH, the interaction of these and a relevant complex, bis(Zn^II-cyclen) (7), has been investigated with a series of polynucleotides, single-stranded poly(U) and poly(G), and double-stranded poly(A)·poly(U), poly(dA)·poly(dT) and poly(dG)·poly(dC). These Zn^II-cyclen complexes interact with the imide-containing nucleobases in the single-stranded poly(U), unperturbed by the presence of the anionic phosphodiester backbone. The affinity constant of 1 for each N(3)-deprotonated uracil base in poly(U) is determined to be log K= 5.1 by a kinetic measurement, which is almost the same as log K=5.2 for the interaction of 1 with uridine. Thus, they disrupt the A-U (or A-T) hydrogen bonds to unzip the duplex of poly(A)·poly(U) or poly(dA)·poly(dT), as demonstrated by lowering of the melting temperatures (T _m) of poly(A)·poly(U) and poly(dA)·poly(dT) in 5 mM Tris-HCl buffer (pH 7.6, 10 mM NaCl) with increase in their concentrations. The order of the denaturing efficiency is well correlated with that of the 1 : 1 affinity constants for each complex with uracil or thymine;7>3>1. The comparison of circular dichroism (CD) spectra for poly(A)·poly(U), poly(A), and poly(U) in the presence of 3 has revealed a structural change from poly(A)·poly(U) to two single strands, poly(A) and poly(U), caused by 3 binding exclusively to uracils in poly(U). On the other hand, the acridine-pendant cyclen complex 3, which earlier was found to associate with guanine by the Zn^II coordinating with guanine N(7), in addition to the π-π stacking, interacts with guanine in the double helix of poly(dG)·poly(dC) from outside and stabilized the double-stranded structure, as indicated by higher T _m. Received: 31 December 1997 / Accepted: 23 February 1998     

TARGETING OF A701G NUCLEOTIDE AT THE HUMAN ATP1A1 LOCUS USING A RNA/DNA CHIMERA

ABSTRACT

The single base substitution mediated by chimeric RNA/DNA oligonucleotide is a new promising approach of gene therapy for single base mutation diseases. We exploited this approach to render HeLa cells resistant to ouabain by introducing a single base substitution in the alpha 1 subunit of the NA⁺/K⁺ ATPase human gene. The chimeric oligonucleotide was administered to HeLa cells by electroporation and the frequency of ouabain resistant cells determined. The results showed that the chimeric RNA/DNA oligonucleotide failed to enhance the frequency of ouabain resistant cells supporting the controversy about the conflicting results of the technique.     

A calorimetric investigation of the heats of binding of Mg ++ to poly A, to poly U, and to their complexes

The heats of binding of Mg⁺⁺ ions to poly A, poly U, and to their complexes, in the presence of Na⁺ ions, have been measurd calorimetrically. In all cases the heat, ΔH(θ), exhibitis a distinct dependence on the extent of binding, θ, and in the cases of poly A and poly U also on the Na⁺ concentration. The values of ΔH(θ) range from +2 to +3 kcal/mole of Mg⁺⁺ bound at θ = 0 to 1.3 kcal/mole at θ = 0.5 except in poly A where at θ = 0 ΔH(θ) = ?2 to ?3 kcal/mole. This is interpreted as being due to a facilitation of base stacking by the binding of Mg⁺⁺. The extent of facilitation is consistent with current estimates of base stacking. A similar effect but of much smaller magnitude is believed to obtain in poly A poly U. An interpretation of the dependence of ΔH(θ) on θ in terms of simple electrostatic interactions, but neglecting solvent effects, was attempted and found to be inadequate.     

Molecular Mechanics Studies of Dinucleoside Methylphosphonates: Influence of Methylphosphonate and its Chirality on the Phosphodiester Conformation

Abstract

Molecular mechanics studies are performed on single stranded as well as base paired forms of dinucleoside methylphosphonates comprising different base sequences for both the Sand R-isomers of methylphosphonate (MP). S-MP produces noticeable distortions in the geometry, locally at the phosphate center, and this enables the stereochemical feasibility of compact g^? g^? phosphodiester. Besides, it tends to perturb the conformations around the P- 03′ and glycosyl bonds, causing minor variations in stacking interactions. In single stranded dinucleosides, the gain in adjacent base stacking interaction energies seems to be sufficient to overcome the barrier to P-03′ bond rotation arising due to S-MP…sugar interaction, and this results in transition to a compact phosphodiester (B_I-type) from an initial extended phosphodiester (B_II-type) conformation. Such a thing seems rather difficult in base pair constrained duplexes. Dinucleosides with R-MP behave analogous to normal phosphate duplexes as the methyl group is away from the sugar. It is found that dinucleoside methylphosphonates are energetically less favoured than the corresponding dinucleoside phosphates mainly due to the depletion of contributions from electrostatic attractive interactions involving the base and sugar with the methylphosphonate consequent to the nonionic nature of the latter. Neither S-MP nor R-MP seem to significantly alter the stereochemistry of duplex structure.     

THE UPTAKE OF LOW CONCENTRATIONS OF LITHIUM IONS INTO RAT CEREBRAL CORTEX SLICES AND ITS DEPENDENCE ON CATIONS

—Rat cerebral slices were incubated in oxygenated Krebs-Ringer bicarbonate glucose saline, and the uptake of Li⁺ was measured after periods of 15 s to 5 min. Saturation was not seen within the concentrations of Li⁺ employed (0·5-2·0 mm ). The half-time of the uptake was 7·9 min. At steady state, after 1 h incubation, the concentration of Li⁺ in the tissue was linearly related to that of the medium (0·5-1·5 mm Li⁺) with a concentration ratio of 1·29–1·66. The concentrations of K⁺ and Na⁺ in the slices incubated without Li⁺ were found to be (μmol/g incubated wt, mean ±s.d .) 63·8 ± 9·6 and 96·2 ± 7·8 respectively (n = 28). In the presence of media with 1·5 mm -Li⁺, the K⁺ and Na⁺ in the slices were 56·2 ± 8·8 and 101·0 ± 7·7 respectively (n = 37). The concentration of Li⁺ in the slices, after 1 h incubation, increased in a non linear way as the concentration of K⁺ in the medium was decreased within a range of 0·10 mm -K⁺. In the absence of K⁺ in the medium the uptake of Li⁺ was approx 50% higher than in the presence of 4·9 mm -K⁺. There was an inverse linear relationship between the concentration of Li⁺ in the slices and that of Ca²⁺ in the medium within the range of 0-5·2 mm (-0·13 mm -Li⁺/mm Ca²⁺). The concentration of Li⁺ in the slices increased by approx 10% when the Mg²⁺ in the medium was increased from 1·3 mm to 2·6 mm . Changes of the concentration of Na⁺ between 120 mm and 170 mm in the medium had no significant effect on the Li⁺ uptake.     

Circular dichroism evidence for G·U and G·T base pairing in poly[r(G-U)] and poly[d(G-T)]

We have measured the circular dichroism (CD) and absorption properties of poly[r(G-U)] and poly [d(G-T)] over a wide range of Na⁺ concentrations and temperatures. We find evidence for self-complexed forms of these polymers at lower temperatures and/or higher Na⁺ concentrations than generally needed for double-strand formation in other DNA and RNA polymers. These self-complexes could be composed of double-stranded regions with weak G·U or G·T base pairs.     

白花泡桐优树组织培养及产业化快繁技术

以自选育的白花泡桐优树茎段为外植体,进行种苗组培快繁技术研究。结果表明:其最佳的外植体灭菌方法是以0.1%升汞处理7 min;合适的初代诱导培养基为MS+6-BA 2.0 mg·L~(-1)+IBA 0.2 mg·L~(-1)+糖30 g·L~(-1)+琼脂3.5 g·L~(-1)(pH 5.8),培养30 d,芽诱导率70%;合适的继代增殖方法为在高浓度植物生长物质培养基MS+6-BA 4.0 mg·L~(-1)+IBA 0.4 mg·L~(-1)+蔗糖30 g·L~(-1)+琼脂3.5 g·L~(-1)(pH 5.8)和低浓度植物生长物质培养基MS+6-BA 0.4 mg·L~(-1)+IBA 0.04 mg·L~(-1)+蔗糖30 g·L~(-1)+琼脂3.5 g·L~(-1)(pH 5.8)中交替培养,获得的丛生芽长势良好,玻璃化率低于5%,增殖系数大于6.0/25 d;最适的生根培养基为1/2MS+NAA0.2 mg·L~(-1)+蔗糖20 g·L~(-1)+卡拉胶3.4 g·L~(-1)(pH 5.8),培养14 d,得到白花泡桐生根苗,每株长根5~10条,根长3~5 cm,生根率98%,根系洁白、根毛少而短,易于清洗。将生根苗按照常规方法炼苗后移栽于温室大棚中,50 d后即可出圃,此时平均苗高1.0 m、地径1.0~2.0 cm,成活率在90%以上。     

Effect of Coordinated Ions on Structure and Flexibility of Parallel G-quadruplexes: A Molecular Dynamics Study

Abstract

Single tract guanine residues can associate to form stable parallel quadruplex structures in the presence of certain cations. Nanosecond scale molecular dynamics simulations have been performed on fully solvated fibre model of parallel d(G₇) quadruplex structures with Na⁺ or K⁺ ions coordinated in the cavity formed by the O6 atoms of the guanine bases. The AMBER 4.1 force field and Particle Mesh Ewald technique for electrostatic interactions have been used in all simulations. These quadruplex structures are stable during the simulation, with the middle four base tetrads showing root mean square deviation values between 0.5 to 0.8 Å from the initial structure as well the high resolution crystal structure. Even in the absence of any coordinated ion in the initial structure, the G-quadruplex structure remains intact throughout the simulation. During the 1.1 ns MD simulation, one Na⁺ counter ion from the solvent as well as several water molecules enter the central cavity to occupy the empty coordination sites within the parallel quadruplex and help stabilize the structure. Hydrogen bonding pattern depends on the nature of the coordinated ion, with the G-tetrad undergoing local structural variation to accommodate cations of different sizes. In the absence of any coordinated ion, due to strong mutual repulsion, O6 atoms within G-tetrad are forced farther apart from each other, which leads to a considerably different hydrogen bonding scheme within the G-tetrads and very favourable interaction energy between the guanine bases constituting a G-tetrad. However, a coordinated ion between G-tetrads provides extra stacking energy for the G-tetrads and makes the quadruplex structure more rigid. Na⁺ ions, within the quadruplex cavity, are more mobile than coordinated K⁺ ions. A number of hydrogen bonded water molecules are observed within the grooves of all quadruplex structures.     

Crystal Structure of 2′-Deoxycytidine Hemidihydrogenphosphate Reveals C+·C Base Pairs and Tight,Hydrogen-Bonded (H2PO4 −)∞ Columns (1)

Abstract

2′-Deoxycytidine hemidihydrogenphosphate has been crystallized in the hexagonal space group P6₂ with α=25.839(3), c = 12.529(1) Å. The structure has been solved using the Patterson search method. The asymmetric unit contains two protonated, base-paired 2′-deoxycytidine dimers and two H₂PO₄ ^? anions. The C⁺·C base pairs are composed of a protonated and a neutral species each and are triple H-bonded, the central N(3)…N(3) bonds being 2.850(7) and 2.884(5) Å. The conformations of the four nucleosides fall in the same category (sugar puckers 2·-endo, glycosidic links anti) but in one of them the glycosidic torsion angle is quite low with consequences in other geometrical parameters. The H₂PO₄ ^? anions are located on twofold axes and form two types of tight columns with P…P separations about 4.18 Å The neighboring units along a column are linked via two very short O…H…O hydrogen bonds (O…O about 2.49 Å) leading to effective equalization of the P-O bonds. The base pairs of the two dC⁺·dC cations are coplanar and form layers perpendicular to the phosphate columns repeating every c/3. Within the layers, the dimers form a network through 0(5′)…O(2) hydrogen bonds but their primary intermolecular interactions have the form of H-bond anchors [N(4)-H…O-P and 0(3′)-H…O-P] to the phosphate groups.     

Crystal Structure of 1-(2′,3′,5′-Tri -O-Acetyl-β-D-ribofuranosyl)-3-acetoxy-2-pyridone: An Antitumour Agent

Abstract

1–C3′, 3′, 5′–Tri—O—acetyl— β—D—ribof uranosyll)—3—acetoxy —2—pyridone,crystallised in space group P2 with z=2 and cell parameters a=12. 446(2), b=10. 415(2), c=7. 600(2) A, β=03. 3O(4). The structure was solved by direct methods and refined by full—matrix least—squares to a final R value of 0·251 for 1847 observed reflections. The sugar—pucker is found to be ³ECC3′ endo) with P = 17.7° and x_CN=170. 2(2)° in the range. The C4′-C5′ conformation is gauche minus. Because of the absence of H—bond donor atoms. the crystal structure is stabilised by a network of C-H—-O close contacts. No base stacking is observed.