The nature of different influence of Cd<Superscript>2+</Superscript> ions on the conformational equilibrium of triple-stranded polyribonucleotides poly(U)•poly(A)•poly(U) and poly(I)•poly(A)•poly(I) in aqueous solutions

The influence of Cd²⁺ ions on the conformational equilibrium of single-stranded (poly(U), poly(A), poly(I)) and triple-stranded polyribonucleotides (A2I, A2U) in aqueous solutions (0.1 M Na⁺ pH 7) has been investigated using difference UV spectroscopy and thermal denaturation. Analysis of the shape and intensity of the DUV spectra of poly(A), poly(I), and A2I has revealed the presence of two types of complex formed as a result of (i) interaction between Cd²⁺ and the N7 atoms of purines, producing macrochelates; and (ii) binding of Cd²⁺ to the N1 atoms of poly(A) and poly(I). Since Cd²⁺ ions are not bound to heteroatoms of the bases in A2U, the conformation of the structure remains stable up to 0.02 M Cd²⁺. There is a critical Cd²⁺ concentration (～1.5?10^?4 M) above which A2I assumes a new helical conformation with lower thermal stability. It is supposed that, upon the formation of the “metallized” A2I triplex, the Cd²⁺ ions are located inside the triple helix and form bridges between the hypoxanthine and adenine of the homopolynucleotide strands.     

Mg2+ and Ni2+ ion effect on stability and structure of triple poly I.poly A.poly I helix

The effects of Mg2+ and Ni2+ ions on the absorption spectra of IMP, single-stranded poly I and three-stranded A2I in solutions with 0.1 M Na+ (pH 7) have been studied. In contrast to Mg2+ ions, the Ni2+ ions affect the absorption spectra of these polynucleotides and IMP. The concentration dependences of the intensity at the extrema in the differential UV spectra suggest that in the region of high Ni2+ concentrations ionic complexes with poly I and A2I are formed, which are characterized by the association constants K'I = 2000 M(-1) and K'A2I = 550 M(-1), respectively. The shape of the DUV spectra prompts the conclusion that these complexes are formed due to the inner-sphere interaction of Ni2+ ions with N7 of poly I and A2I presumably due to the outer-sphere Ni2+-O6 interaction. The formation of the complexes leads to destruction of A2I triplexes. The dependences of the melting temperature (T(m)) of A2I on Mg2+ and Ni2+ concentrations have been measured. The thermal stability is observed to increase at the ionic contents up to 0.01 M Mg2+ and only to 2x10(-4) M Ni2+. At higher contents of Ni2+ ions, T(m) lowers and the cooperativity of A2I melting decreases continuously. In all the cases the melting process is the A2I-->A+I+I (3-->1) transition. According to the "ligand" theory, these effects are generated by the energy-advantageous Ni2+ binding to single-stranded poly I (K'A2I < K'I) and by the greater number of binding sites which appears during the 3-->1 transition and is entropy-advantageous.     

Interaction of divalent metal ions with four-stranded polyriboinosinic acid

Interaction of Mg2+, Ca2+, Cu2+ ions with the four-stranded poly(I) was studied using differential UV and visible spectroscopies. It was shown that, up to concentrations of approximately 0.1 M, Mg2+ and Ca2+ ions do not bind to heteroatoms of hypoxanthine of the four-stranded poly(I). Cu2+ ions interact with N7 (and/or N1) and O6 (through the water molecule of the hydrate shell of the ion). The latter seems to induce the enolization of hypoxanthine the deprotonation of N1, and, as a result, the transition of the four-stranded helix to single-stranded coils. Single-stranded chains form compact particles with an effective radius of about 100 A.     

Binding of divalent copper and calcium ions to poly I

The effect ot Cu²⁺ and Ca²⁺ ions, on the ultraviolet differential (UVD) spectra of single-stranded poly I was studied and the coordination (Δε_b) and conformation (Δε_c) conponents of the spectra calculated The comparison of Δε_b and the UVD spectrum of protonated IMP leads to the conclusion that N(7) ot inosine-5'-monophosphate (IMP) is a coordinating site tor Ca²⁺ and Cu²⁺ ions on the polymer bases. The binding ot Ca²⁺ and Cu²⁺ ions causes differently directed displacements of the four absorption bands of poly I, which are observed in the wavenumber range (50-34) × 10³ cm⁻¹ The calculation of concentration dependencies tor the association constants (K“) ot Ca²⁺ and Cu²⁺ ions binding to poly I bases shows that the binding is cooperative The K“ values for the poly I + Ca²⁺ complex are two orders of magnitude lower than those for the poly 1 + Cu²⁺ complex At low ion concentrations, binding to the poly I phosphates predominates and increases the degree of the polynucleotide helicity. At higher concentrations the spectra are mainly affected by the ion binding to bases, which results in melting of the helical parts of poly I At Ca²⁺ concentrations exceeding 10⁻³ M light-scattering aggregates are formed. The degree of monomer order in them is close to that observed in multistranded helices of poly I     

Raman spectroscopic study of the effects of Ca2+, Mg2+, Zn2+, and Cd2+ ions on calf thymus DNA: binding sites and conformational changes

The interaction of Mg2+, Ca2+, Zn2+, and Cd2+ with calf thymus DNA has been investigated by Raman spectroscopy. These spectra reveal that all of these ions, and particularly Zn2+, bind to phosphate groups of DNA, causing a slight structural change in the polynucleotide at very small metal: DNA (P) concentration ratio (ca. 1:30). This results in increased base-stacking interactions, with negligible change of the B conformation of DNA. Contrary to Zn2+ and Cd2+, which interact extensively with the nucleic bases (particularly at the N7 position of guanine), the alkaline-earth metal ions are bound almost exclusively to the phosphate groups. The affinity of both the Zn2+ and Cd2+ ions for G.C base pairs is comparable, but the Cd2+ ions interact more extensively with A.T pairs than Zn2+ ions. Interstrand cross-linking through the N3 atom of cytosine is suggested in the presence of Zn2+, but not Cd2+.     

Mg2+ ion effect on conformational equilibrium of poly A . 2 poly U and poly A poly U in aqueous solutions

Differential UV spectroscopy and thermal denaturation were used to study the Mg²⁺ ion effect on the conformational equilibrium in poly A · 2 poly U (A2U) and poly A · poly U (AU) solutions at low (0.01 M Na⁺) and high (0.1 M Na⁺) ionic strengths. Four complete phase diagrams were obtained for Mg²⁺–polynucleotide complexes in ranges of temperatures 20–96 °C and concentrations (10⁻⁵–10⁻²) M Mg²⁺. Three of them have a ‘critical’ point at which the type of the conformational transition changes. The value of the ‘critical’ concentration ([Mg_t²⁺]_cr=(4.5±1.0)×10⁻⁵ M) is nearly independent of the initial conformation of polynucleotides (AU, A2U) and of Na⁺ contents in the solution. Such a value is observed for Ni²⁺ ions too. The phase diagram of the (A2U+Mg²⁺) complex with 0.01 M Na⁺ has no ‘critical’ point: temperatures of (3→2) and (2→1) transitions increase in the whole Mg²⁺ range. In (AU+Mg²⁺) phase diagram at 0.01 M Na⁺ the temperature interval in which triple helices are formed and destroyed is several times larger than at 0.1 M Na⁺. Using the ligand theory, a qualitative thermodynamic analysis of the phase diagrams was performed.     

The binding of Mg(II) and Ni(II) to synthetic polynucleotides

Equilibria and kinetics of the interactions of Mg2+ and Ni2+ with poly(U), poly(C) and poly(I) have been investigated at 25 degrees C, an ionic strength of 0.1 M, and pH 7.0 or 6.0. Analogous studies involving poly(A) were reported earlier. All binding equilibria were studied by means of the (usually small) absorbance changes in the ultraviolet range. This technique yields apparent binding constants which are fairly large for the interaction of Ni2+ with poly(A) (K = 0.9 X 10(4) M-1) and poly(I) (K approximately equal to 2 X 10(4) M-1) but considerably lower for the corresponding Mg2+ systems, Mg2+-poly(A) (K = 2 X 10(3) M-1) and Mg2+-poly(I) (K = 280 M-1). Each of the two pyrimidine nucleotides binds both metal ions with about the same strength (K approximately equal to 65 M-1 for poly(U) and K near 600 M-1 for poly(C]. In the case of poly(C) the spectral changes deviate from those expected for a simple binding equilibrium. In addition, the binding of Ni2+ to the four polynucleotides was measured by using murexide as an indicator of the concentration of free Ni2+. The results obtained by this technique agree or are at least consistent with those derived from the ultraviolet spectra. Complications are encountered in the binding studies involving poly(I), particularly at higher metal ion concentrations, obviously due to the formation of aggregated poly(I) species. Kinetic studies of the binding processes were carried out by the temperature-jump relaxation technique. Measurable relaxation effects of time constants greater than 5 microseconds were observed only in the systems Ni2+-poly(A) and Ni2+-poly(I). Such not-too-fast reaction effects are expected for processes which include inner-sphere substitution steps at Mg2+ or Ni2+. The relaxation process in Ni2+-poly(I) is characterized by (at least) four time constants. Obviously, the complicated kinetics again include reactions of aggregated poly(I). The absence of detectable relaxation effects in all other systems (except Mg2+-poly(I), the kinetics of which was not investigated) indicates that inner-sphere coordination of the metal ions to specific sites of the polynucleotides (site binding) does not occur to a significant extent. Rather, the metal ions are bound in these systems mainly by electrostatic forces, forming a mobile cloud. The differences in binding strength which are nevertheless observed are attributed to differences in the conformation of the polynucleotides which result in different charge densities.     

Interaction of metal ions with polynucleotides and related compounds. IX. Unwinding and rewinding of poly(A + U) and poly(I + C) by copper(II) ions

It is demonstrated that, poly(A + U) and poly(I + C) are both formed under low ionic strength conditions. Continuous variation studies indicate the formation of copper(II) complexes of poly A, poly C, and poly I, but not of poly U. Copper(II) in a 1:1 ratio to polynucleotide prevents the formation of poly(A + U) and brings about the dissociation of the poly (A + U) complex produced in the absence of the metal. Poly (I + C) is similarly dissociated by copper(II) ions. The addition of sufficient electrolyte reverses the copper(II) induced dissociation of poly(I + C). The effect of copper(II) on ordered synthetic polynucleotides is thus very similar to its effect on DNA.     

Left-handed helical structure of poly[d(A-C)].poly[d(G-T)] studied by infrared spectroscopy

Infrared spectroscopic studies demonstrate the ability of poly[d(A-C)].poly[d(G-T)] to adopt a Z-type conformation. The Z form of the unmodified polynucleotide is induced by Ni2+ counterions and not by Na+. The B----Z equilibrium is shifted at room temperature, in the presence of 1 Ni2+/nucleotide, by an increase in the concentration of poly[d(A-C)].poly[d(G-T)]. The importance of specific binding of Ni2+ ions on the N7 site of purines in the stabilization of the Z form is also discussed.     

Evaluation of the metal-ion-coordinating differences between the 2'-, 3'- and 5'-monophosphates of adenosine

The stability constants of the 1:1 complexes formed between Mg2+, Ca2+, Sr2+, Ba2+, Mn2+, Co2+, Ni2+, Cu2+, Zn2+ or Cd2+ and 2'AMP2-, 3'AMP2- or 5'AMP2- were determined by potentiometric pH titration in aqueous solution (I = 0.1 M, NaNO3; 25 degrees C). The experimental conditions were carefully selected such that self-association of the nucleotides and their complexes is negligibly small; i.e. it was made certain that the properties of the monomeric divalent-metal-ion--AMP [M(AMP)] complexes were studied. Based on recent measurements with simple phosphate monoesters, R-MP2- where R is a non-coordinating residue [Massoud, S. S. & Sigel, H. (1988) Inorg. Chem. 27, 1447-1453], it is shown that all the M(AMP) complexes of the alkaline earth ions, with the possible exception of Mg(5'AMP), have exactly the stability expected for a sole-phosphate coordination of the metal ion. The same property is revealed for the complexes with Mn2+, Co2+, Zn2+ or Cd2+ and 3'AMP2-; in case of Ni(3'AMP) and Cu(3'AMP) a slight stability increase just at the edge of the experimental-error limits is indicated. This slight stability increase is attributed to the formation of a macrochelate (possibly with N-3); in fact, additional information confirms macrochelation for Cu(3'AMP). About 45% of Cu(2'AMP) exists in aqueous solution as a macrochelate (probably involving N-3); the other M(2'AMP) complexes (M2+ = Mn2+, Co2+, Ni2+, Zn2+, Cd2+) form (if at all) only traces of a base-backbound species. Most pronounced is macrochelate formation with 5'AMP2-: all mentioned 3d ions and Zn2+ or Cd2+ form to some extent macrochelates via N-7 (the structures of these closed species are indicated). In case of M(5'AMP) the base-binding site is certain: replacement of N-7 by a CH unit (tubercidin 5'-monophosphate) eliminates any increased complex stability, whereas formation of the 1,N6-etheno bridge to form 1,N6-ethenoadenosine 5'-monophosphate results in the phenanthroline-like N-6,N-7 site which facilitates macrochelation significantly.     

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).     

Interaction of DNA with divalent metal ions

The interaction between the native DNA macromolecules and Ca2+, Mn2+, Cu2+ ions in solutions of low ionic strength (10(-3) M Na+) is studied using the methods of differential UV spectroscopy and CD spectroscopy. It is shown that the transition metal ions Mn2+ exercise binding to the nitrogen bases of DNA at concentrations approximately 5 x 10(-6) M and form chelates with guanine of N7-Me(2+)-O6 type. Only at high concentrations in solution (5 x 10(-3) M) do Ca2+ ions interact with the nitrogen bases of native DNA. In the process of binding to Ca2+ and Mn2+ the DNA conformation experiences some changes under which the secondary structure of the biopolymer is within the B-form family. The DNA transition to the new conformation is revealed by its binding to Cu2+ ions.     

Z form of poly d(A-C).poly d(G-T) in solution studied by Raman spectroscopy.

Poly d(A-C).poly d(G-T) structures have been studied in solution by Raman spectroscopy, in presence of Na+, Mn2+ and Ni2+ counterions. Increase of the Na+ concentration or addition of Mn2+ ions up to 1M MnCl2 does not modify the B geometry of the polynucleotide. On the contrary, in conditions of low water activity (4M NaCl), the presence of small amounts of nickel ions (65 mM) induces a left-handed geometry of the DNA. The shift of the guanine line located at 682 cm-1 in B form to 622 cm-1 reflects unambiguously the C2'-endo/anti-greater than C3'-endo/syn reorientation of the deoxyribose-purine entities. Moreover modifications in the phosphate backbone lines indicate that the polymer is in a Z conformation. New or displaced lines corresponding to adenosine vibrations are correlated with the left-handed structure. An interaction of the Ni2+ ions specifically with the N7 site of purines, combined with a low water activity is necessary to promote the B-greater than Z transition.     

Interaction of metal ions with polynucleotides and related compounds. XXII. Effect of divalent metal ions on the conformational changes of polyribonucleotides

Changes in the conformation of poly(G), poly(C), poly(U), and poly(I) in the presence of divalent metal ions Mg²⁺, Ca²⁺, Mn²⁺, Co²⁺, Ni²⁺, Cu²⁺, Cd²⁺, and Zn²⁺ have been measured by means of ORD and u.v. spectra. Mg²⁺ and Ca²⁺ ions stabilize helical structures of all the polynucleotides very effectively at concentrations several orders of magnitude lower than the effective concentration of Na⁺ion. Cu²⁺ and Cd²⁺ destabilize the helical structure of polynucleotides to form random coils. Zn²⁺, Ni²⁺, Co²⁺, and Mn²⁺ions do not behave in such a clear-cut manner: they selectively stabilize some ordered structures, while destabilizing others, depending on the ligand strength of the nucleotide base as well as the preferred conformation of that polynucleotide.     

Interaction of Ag+ ions with DNA and its monomers

Differential UV spectra of DNA and its monomers that were induced by Ag+ ions were measured, and the effect of ions on the parameters of the helix-coil transition was studied. The data obtained confirm the existence of "strong" and "weak" modes of binding of Ag+ to DNA. The earlier proposed proton transfer from N1G to N3C, which is determined by the interaction of Ag+ with N7G (a "strong" complex), follows immediately from the shape of the differential UV spectra. The positive cooperativity of the binding of Ag+ to DNA upon the formation of a "weak" complex is due to the cooperativity of the transition of DNA to a new double-helical conformation. A model of this conformation is proposed which suggests the formation of Hougsteen GC and AT pairs.     

Induction of helicity in polyuridylic acid and polyinosinic acid by silver ions

Silver ions binding to poly(U) and poly(I) produce highly ordered multistranded helices under conditions which would otherwise lead to random coils. Evidence for helicity comes from the hypochromicity and high ellipticity generated in the polymers by Ag⁺ binding, as well as from x-ray studies and from the cooperativity of the Ag⁺ complexing reaction. Continuous variation studies show that both polymers form 1:1 and 2:1 polymer–Ag⁺ complexes. Low pH favors the 1:1 complex with poly(U) and the 2:1 complex with poly(I); the reverse is true at high pH. Ag⁺ binding and proton-release experiments make it clear that at low pH, unprotonated electron-donor groups are complexed preferentially, but that at high pH, Ag⁺ readily displaces H⁺ from protonated groups. In poly(I) the unprotonated donor is N(7), leading at low pH to a 2:1 complex containing N(7)-Ag-N(7) bonds; at high pH, proton release from N(1) leads to a 1:1 complex containing N(1)-Ag-O bonds. In poly(U) there is no unprotonated donor; the low-pH 1:1 complex involves deprotonation of only one N(3) per bound Ag⁺, leading to N₃-Ag-O bonding, while high pH causes deprotonation of two N(3) per Ag⁺ and a 2:1 N(3)-Ag-N(3) complex. Thus silver ions react with the nucleotide bases in chemically predictable ways, and the formation of different Ag–nucleotide bonds leads to different multiple-helix structures.     

Studies of calcium ion binding to poly A

Ultraviolet differential spectra of poly A we studied in the presence of Ca2+ ions with 10(-3)M Na+ in the solution. At concentrations lower than 10(-3)M Ca2+, the ions bind to phosphate groups of the single helical polymer, thus increasing its degree of helicity. At higher concentrations, the ions start binding to the bases of poly A, producing aggregates whose effective radius, as found with an electric microscope, is not more than 10(2) A. These particles stack to form aggregates of an order-of-magnitude higher size. The mutual orientation of bases in the poly A aggregates is of a high degree of order. The calculation of concentration dependences of Ca2+-poly A binding constants shows that this process is cooperative.     

B-X transition in synthetic and natural (dA-dT)n.(dA-dT)n sequences

AB-X transition of polyh(dA-dT).poly(dA-dT) was observed to occur in methanol-water mixtures with methanol concentrations higher than 50% in the presence of a specific combination of monovalent and divalent cations. In the presence of Na+, divalent cations induce denaturation of poly(dA-dT).poly(dA-dT) accompanied by condensation and/or aggregation, and effect similar to that observed previously with random sequence DNA (Votavová, Kucerová, Felsberg and Sponar, J. Biomol. Struct. Dyn. 4,477-489, 1986). In the presence of Cs+ cations a B-X transition was induced by addition of Ca2+ or Mn2+ but not Mg2+ or Ni2+ ions. Circular dichroism and ultraviolet spectroscopy demonstrate that the X conformation is a double stranded form of poly(dA-dT).poly(dA-dT) belonging presumably to the B family which, however has an altered base stacking. The X conformation of poly(dA-dT).poly(dA-dT) found in methanol-water mixtures is a condensed and/or aggregated form. In contrast, the X conformation characterized by similar CD spectra observed in high salt concentrations is not aggregated up to a concentration of 6 M CsF. In methanol-water mixtures (A+T)-rich bacterial DNA behaves essentially as a random sequence DNA revealing no detectable amount of the X form. On the other hand crab (Cancer pagurus) satellite and crab non-satellite DNAs containing varying amounts of (dA-dT)n.(dA-dT)n sequences were shown to undergo a B-X transition, at least partly, in both methanol-water mixtures and 6 M CsF solutions.     

Electro-optical studies of conformation and interaction of polynucleotides

Measurements by the technique of electric birefringence with pulsed sinusoidal electric fields on polyriboadenylic acid (poly-A) and polyribouridylic acid (poly-U) indicate that the kinetics of the double-stranded helix formation of poly (A + U) in the presence of Mg²⁺ is second order and consists of two steps: nucleation and propagation of base pairs from nuclei. The nucleation involves approximately 7 base pairs. It seems that the requirement of 7 base pairs to start the formation of a double-stranded helix is not peculiar to poly (A + U) but is associated with double-stranded helices of polynucleotides in general. This implies that it may be associated with spatial requirements of the phosphate-sugar backbone, rather than with the particular bases linked to the backbone. The decline in rate of poly (A + U) formation observed above a critical temperature is the consequence of changes in the poly-A conformation setting in at this critical temperature, rather than resulting from an increase in the reversibility of the base-pair propagation step of double-stranded helix formation. The dominant role of the conformation of poly-A in the double-stranded helix formation of poly (A + U) is further borne out by the pH dependence of the rate which completely parallels the conformation changes known to occur in poly-A as a function of pH. This indirectly suggests that at neutral pH poly-A is a single-stranded helix. The rotary diffusion coefficients attest to the flexibility of this helix, while the stacked nature of the base pairs at low temperatures is revealed by the identical increments in the specific Kerr constant on going from poly-A to poly (A + U) and from poly (A + U) to poly (A + 2U) helices. Results suggest that Mg²⁺ binds to the phosphate part of the backbone. Poly-U binds Mg²⁺ more strongly than poly-A; this difference in binding strength is attributed to differences in conformation (random coil versus helix). It is also borne out by the present results that the degree of order in the structure of poly-U, even at low temperatures and neutral pH, is at best an order of magnitude smaller than that of poly-A under similar conditions. Furthermore, the earlier proposed double-stranded structure of poly-U is called into question. A hairpinlike structure seems to agree with results of this investigation. Finally, the results support the contention that the ion atmosphere polarization is responsible for orientation of polyelectrolytes in the presence of alternating electric fields in the neighborhood of 25 kc./sec. frequency.