Topography of nucleic acid helices in solutions. 3. Interactions of spermine and spermidine derivatives with polyadenylic-polyuridylic and polyinosinic-polycytidylic acid helices

The synthesis of spermine derivatives (II), \documentclass{article}\pagestyle{empty}\begin{document}$ {\rm R}_1 {\rm R}_{\rm 2} {\rm R}_{\rm 3} \mathop {\rm N}\limits^ + \left( {{\rm CH}_2 } \right)_3 \mathop {\rm N}\limits^ + {\rm R}_{\rm 1} {\rm R}_{\rm 2} \left( {{\rm CH}_2 } \right)_2 ]_2 \cdot 4{\rm X}^ - $\end{document}, and spermidine derivatives (III), \documentclass{article}\pagestyle{empty}\begin{document}$ {\rm R}_1 {\rm R}_{\rm 2} {\rm R}_{\rm 3} \mathop {\rm N}\limits^ + \left( {{\rm CH}_2 } \right)_4 \mathop {\rm N}\limits^ + {\rm R}_{\rm 1} {\rm R}_{\rm 2} \left( {{\rm CH}_2 } \right)_3 \mathop {\rm N}\limits^ + {\rm R}_{\rm 1} {\rm R}_{\rm 2} {\rm R}_3 \cdot 3{\rm X}^ - $\end{document}, are reported. The effects of these salts on the helix–coil transition of rA–rU and rI–rC helices were examined. Increasing the size of the hydrophobic substituents, R¹, R², and R³ lowers the degree of stabilization of the helical structure. The disproportionation reaction, 2rA–rU→rA–rU₂ + rA occurs readily with salts II and III, especially when the substituents, R₁, R₂, and R₃ are small, i.e., H or Me. Spermine is found to stabilize the rA–rU² and rI–rC helices to approximately the same extent; however, large differences between the degree of stabilization of rA–rU₂ and rI-rC helices are observed when the substituents R₁, R₂, and R₃ are large hydrophobic groups. Similar results are also obtained for the spermidine series. Finally, differences in the interactions of the salts II and III with rA–rU₂ and rI–rC helices suggest that the latter helix is denser.     

Topography of nucleic acid helices in solutions. The interaction specificities of optically active amino acid derivatives

The synthesis and interactions of the d- and l-enantiomers of the amino acid amide derivatives [Formula: see text] (I) and lysyl dipeptides [Formula: see text] (II) with poly rI.poly rC, poly rA.poly rU and calf thymus DNA is reported. The following results were found. (1) The degree of stabilization of the helices as measured by the T(m) (;melting' temperature) of the helix-coil transition was dependent on the nature of the amino acid. (2) For the poly rI.poly rC helix, the l-enantiomers of salts (I) and (II) stabilized more than the d-enantiomers. The same was true for calf thymus DNA in the presence of salts (II) and for poly rA.poly rU in the presence of salts (II) and the proline derivatives of salts (I). (3) As R increased in size and became more apolar, the amount of stabilization of the poly rI.poly rC helix in the presence of salts (I) decreased. On the other hand, the amount of stabilization increased with more polar substituents. An attempt was then made to determine whether the difference in stabilization of the double-stranded helices at the T(m) in the presence of the l- and d-enantiomers of salts (I) is due to the interaction with the helix, the random coil or both. A new method was developed for determining the binding of small ions to polyions that involves a competition between an insoluble polystyrene ion-exchange resin and the soluble polyion for the counterion. Dissociation constants are obtained for the complexes of single- and double-stranded helices with the salts (I). The results are illuminating and indicate that with certain helices, i.e. poly rA.poly rU, the interactions of salts (I) with the single strands may not be ignored. It is concluded that the high optical specificity found in Nature, i.e. d-ribose in nucleic acids and l-amino acids in proteins, cannot be attributed solely to monomer-polymer interactions described by Gabbay (1968).     

Topography of nucleic acid helices in solutions. 28. Evidence for a dynamic structure of DNA in solution

Proton magnetic resonance (pmr), ultraviolet absorption, induced circular dichroism (CD), and viscometric evidence is presented which show that reporter molecules $\text{1}$ and $\text{2}$ bind to DNA via an intercalation process. Preliminary kinetic studies show that the DNA·$\text{1}$ complex forms rapidly (i.e., <1 msec), whereas the DNA·$\text{2}$ complex forms at a considerably slower rate ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{> 100 msec}$). The kinetic results, and the steric requirements for intercalation of $\text{2}$ can be explained on the basis of a dynamic structure of DNA.     

Topography of nucleic acid helices in solutions. XXIV. Intercalation specificities of DNA and their possible role in the recognition process

Through the use of reporter molecules, I, it is shown that more than one type of intercalating site must exist in DNA. Although this finding is completely consistent with the DNA structure it has not yet been demonstrated. The significance of the presence of different intercalating sites in DNA may be of extreme importance in the recognition of nucleic acid-protein systems.     

Topography of nucleic acid helices in solutions. II. Structure of the double-stranded rA-rU, rI-rC, acid rA, and the triple-stranded rA-rU2 and rA-rI2 helices

Information concerning the structures of rA–rU, rA–rU₂ rI–rC, rA–rI₂, and acid rA helices in solutions is reported. Through the use of diquaternary ammonium salts of the general structure, \documentclass{article}\pagestyle{empty}\begin{document}$ {\rm R}_1 {\rm R}_2 {\rm R}_3 \mathop {\rm N}\limits^ + ({\rm CH}_2 )n\mathop {\rm N}\limits^ + {\rm R}_1 {\rm R}_2 {\rm R}_3 \cdot 2{\rm Br}^ - $\end{document} (I), it is shown that (1) the distances between adjacent negatively charged oxygen atoms on the helix increases in the following order rA–rI₂ < rI–rC < rA–rU ? rA–rU₂; (2) the density of the helices increases in the order. rA–rI₂ < rA–rU < rA–rU₂ < rI–rC; (3) there is a large hydrophobia site in rA–rI₂ and possibly also in rA–rU, rA–rU₂, and rI–rC helices; (4) the results of the interactions between the salts of type I and the helices may be formulated in semi-quantitative terms by the use of two parameters, α, and β which are shown to be related to the charge separation and the density of the helices, respectively; (5) the studies in solutions compare favorably with the x-ray studies on the fibers; and (6) the acid rA helix differs significantly from the other helices by the fact that the electrostatic interstrand interactions between the negatively charged oxygen atom of a phosphate group and the positively charged 10-amino group of adenine contribute significantly to the stabilization of the helix, and thus it is found that the presence of the salts, I, leads to a significant destabilization of the acid rA helix.     

Quasielastic light-scattering study of polyadenylic acid solutions. II

Quasielastic light scattering is used to study saline solutions of polyadenylic acid with varying polymer concentrations and molecular masses. These experiments clearly show the existence of two relaxation times. For dilute solutions, when the chains are mutually independent, the fast mode is due to the free diffusion of the polymer chains. For concentrations above the overlap concentration C*, the fast mode is due to the propagation of collective excitations of the pseudolattice of polymer chains. The slow modes are observed when the polymer concentration is in the vicinity of the overlap concentration C*. A series of experiments shows that both their relaxation time and amplitude depend only on the polymer concentration and not on the polymer molecular mass. This result rules out any previous explanation based on individual chain motion. Furthermore, since the amplitudes depend on the time elapsed from the preparation of the solution, the slow modes are due to the diffusion of concentration inhomogeneities in the pseudolattice.     

Ring current shielding effects in nucleic acid double helices.

Values of ring current shielding in parts-per-million have been calculated for double helical nucleic acids in the A-RNA (RNA-11), A' -RNA (RNA-12) and B-DNA geometries. Atomic coordinates determined previously from x-ray diffraction of fibers were used to calculate the positions of protons relative to both nearest and second nearest neighboring bases, including those on the complementary strand. The magnitude of the diamagnetic shielding was then calculated for each aromatic ring. From these calculations tables were constructed for use in determining the shielding expected for carbon-bound and ring nitrogen-bound protons of any double helical nucleic acid sequence. The results are compared with available experimental data for several oligonucleotides and with previous ring current shielding calculations where differences of up to 0.4 ppm are found.     

Free energy of imperfect nucleic acid helices. II. Small hairpin loops

Physical studies of enzymically synthesized oligonucleotides of defined sequence are used to evaluate quantitatively the stability of small RNA hairpin loops and helices. The series (Ap)₄G(pC) _N(pU)₄, N = 4, 5 or 6, exists as monomolecular hairpin helices when N ≥ 5, and as imperfect dimer helices when N ≤ 4. In this size range, hairpin loops become more favorable (less destabilizing thermodynamically) as they increase in size from 3 to 4 to 5 unbonded nucleotides. Very small hairpin loops are particularly destabilizing; molecules whose base sequence would imply a hairpin loop of three nucleotides will generally exist with a loop of five, including a broken terminal base pair.Thermodynamic parameters for base pair and loop formation are calculated by a method which makes unnecessary the use of measured enthalpies of polynucleotide melting. Literature data on oligonucleotide double helices yield estimates of the free energy contribution from each of the six types of stacking interactions between three possible neighboring base pairs. The advantage of this approach is that the properties of oligonucleotides are used in predicting the stability of small RNA helices, avoiding the long extrapolation from the properties of high polymers.We provide Tables of temperature-dependent free energies that allow one to predict the stability and thermal transition temperature of many simple RNA secondary structures (applicable to ~1 m-Na⁺ concentration). As an example, we apply the rules to an isolated fragment of tRNA^Ser (yeast) (Coutts, 1971), whose properties were not used in calculating the free-energy parameters. The experimental melting temperature of 88 °C is predicted with an error margin of 5 deg. C.     

Thermochemistry of aqueous solutions of alkylated nucleic acid bases. IV. Enthalpies of hydration of 5-alkyluracils

Enthalpies of sublimation, DeltaH degrees (subl) and of solution in water, DeltaH degrees (sol) were determined for a series of crystalline 1,3-dimethyl-uracil derivatives substituted at the C5-ring carbon atom with alkyl groups (-C(n)H(2n+1), n = 2-4) and some of their C(5.6)-cyclooligomethylene analogues (-(CH2)(n)-, n = 3-5). From these data. enthalpies of hydration DeltaH degrees (hydr)= DeltaH degrees (sol) - DeltaH degrees (subl) were calculated and corrected for energies of cavity formation in pure liquid water in order to obtain enthalpies of interaction, DeltaH degrees (int) of the solutes with their hydration shells. The latter are discussed together with the recalculated DeltaH degrees (int) for variously methylated uracils, obtained previously according to a simplified correction procedure, in terms of perturbations in the energy and scheme of hydration of the diketopyrimidine ring brought about by alkyl substitution. It was found that each -CH2-group added with an alkyl substitution contributes favorably about -20 kJ mol(-1) toDeltaH degrees (int).This contribution is partially cancelled by the unfavorable contribution to DeltaH degrees (int) connected with removal of some water molecules bound in the first and subsequent hydration layers by an alkyl substituent. This is particularly evident on substitution at the polar side of the diketopyrimidine ring on which water molecules are expected to be bound specifically.