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.     

DNA interaction with biologically active divalent metal ions: binding constants calculation

In our previous work we have shown that under the action of Cu²⁺, Mn²⁺ and Ca²⁺ ions DNA is able to transit into a compact state in aqueous solution. In the present work we carried out calculations of binding constants for divalent metal ions interacting with DNA in terms of the macromolecule statistical sum. The formula for calculation of the binding constants and cooperativity parameters was proposed. It was shown that on the “coil state”–“compact (globule) state” transition a single DNA molecule may undergo the first-order phase transition while the transition of the assembly of average DNA chains is of sigmoidal character typical of the cooperative and continuous transition.     

Urea effect on Cu(2+)-induced DNA structural transitions in solution

Cu(2+) ion interaction with DNA in aqueous solutions containing urea (0-5 M) was studied by IR spectroscopy. It was shown that upon the Cu(2+) ion binding DNA transition into a compact form occurs. This transition is of positive cooperativity. We suppose that the mechanism of Cu(2+)-induced DNA compaction in solutions containing urea is not completely electrostatic. Urea addition to the DNA solution decreases the Cu(2+) ion concentration required to induce DNA compaction. As the urea content in solution rises, the binding constant of Cu(2+) ions interacting with DNA increases, going through the maximum in the case of 2 M solution; further increase of the urea content in solutions leads to decrease of the binding constant. DNA transition into the compact form under the Cu(2+) ion action is determined not only by the effects of the solution dielectric permeability but by the solvation effects; when changes of the dielectric permeability are small the solvation effects may prevail. Urea addition to the DNA solution also decreases cooperativity of the DNA compaction process. Perhaps, cooperativity of the DNA transition into the compact state depends on the ordered spatial structure of water adjacent to the macromolecule and decreases on the structure destruction.     

On the possibility of true phase transition in heterogeneous DNA during thermal denaturation under conditions close to equal stability of A+T and G+C pairs

The DNA helix–coil transition has been studied in the presence of high concentrations of manganese ions (about 10^?3M), which corresponds to the conditions close to equal stability of the A+T and G+C pairs, at the ionic strengths of 10^?1, 10^?2, and 1.6 × 10^?3M Na⁺. With the Mn²⁺ ion effect, the transition range is significantly reduced to not more than 0.2°C at 1.2 × 10^?3M Mn²⁺ and 1.6 × 10^?3M Na⁺. The melting curves display a sharp kink at the end of the helix–coil transition, which is interpreted as an indication of the second-order phase transition. It is shown that the melting curves obtained can be approximated by a simple analytical expression 1 – θ = exp[–a(t_c - t)], where θ is the DNA helix fraction, t_c is the phase transition temperature, and a is an empirical parameter characterizing the breadth of the melting range and responsible for the magnitude of a jump of the helicity derivative with respect to the temperature at the phase transition point.     

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 3d-and 4d-Group Metal Ions With GMP

Abstract

The interaction of 3d- and 4d- group metal ions with GMP is studied by the differential UV spectroscopy method. Ni²⁺, Co²⁺, Cu²⁺, Zn²⁺, Cd²⁺ form a chelate structure, interacting innerspherically with N7 and outerspherically with O6, while Ag⁺ binds innerspherically to N7 as well as to O6. The difference in association constants for 3d ions binding to GMP is mainly due to differences in the ion radii.     

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.     

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.     

Poly(rA) • Poly(rU) with Ni2+ Ions at Different Temperatures: Infrared Absorption and Vibrational Circular Dichroism Spectroscopy

Abstract

Phase transitions were studied of the sodium salt of poly(rA) ?poly(rU) induced by elevated temperature without Ni²⁺ and with Ni²⁺ in 0.07 M concentration in D₂O (～0.4 [Ni]/[P]). The temperature was varied from 20° C to 90° C. The double-stranded conformation of poly(rA)?poly(rU) was observed at room temperature (20° C—23° C) with and without Ni²⁺ ions. In the absence of Ni²⁺ ions, partial double- to triple-strand transition of poly(rA) ?poly(rU) occurred at 58° C, whereas only single-stranded molecules existed at 70° C. While poly(rU) did not display significant helical structure, poly(rA) still maintained some helicity at this temperature. Ni²⁺ ions significantly stabilized the triple-helical structure. The temperature range of the stable triple-helix was between 45° C and 70° C with maximum stability around 53° C. Triple-to single-stranded transition of poly(rA) ?poly(rU) occurred around 72° C with loss of base stacking in single-stranded molecules. Stacked or aggregated structures of poly(rA) formed around 86° C. Hysteresis took place in the presence of Ni²⁺ 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.     

Complexes of (dG-dC)20 with Mn2+ Ions: A Study by Vibrational Circular Dichroism and Infrared Absorption Spectroscopy

Abstract

The B-Z transition of the synthetic oligonucleotide, (dG-dC)₂₀, induced by Mn²⁺ ions at room temperature, was investigated by absorption and Vibrational Circular Dichroism (VCD) spectroscopy in the range of 1800–800 cm^?1. Metal ion concentration was varied from 0 to 0.73 M Mn²⁺ (0 to 8.5 moles of Mn²⁺ per mole of oligonucleotide phosphate, [Mn]/[P]). While both types of spectra showed considerable changes as the Mn²⁺ concentrations were raised, differences between the two were often complementary in their expression and extent, those displayed by VCD being more clearly evident due to the inversion of the opposite helical sense from the right-handed to the left-handed conformation. The main phase of the transition occurred in the metal ion concentration between 0.8?1.1 [Mn]/[P]. Gradual changes that took place in the spectra were interpreted in terms of simultaneous processes that depended on metal ion concentration, namely B-Z transformation, binding of Mn²⁺ to phosphates and to nitrogen bases, and partial denaturation. Below～0.6 [Mn]/[P], only a small portion of the oligonucleotide adopted the Z conformation within a 3 hour period, whereas conversion was completed in the same time interval for concentrations between 0.9?1.2 [Mn]/[P]. At [Mn]/[P] > 1.7, complete transition to the Z-form took place immediately on adding Mn²⁺. Applying VCD spectroscopy in combination with conventional infrared absorption proved most useful for corroborating changes in the absorption spectra, and for detecting in an unique manner, not attainable by absorption methods, conformational changes that lead to the inversion of the helical sense of the oligonucleotide.