Z helix-coil transition of d(C-Br8G-C-G-C-Br8G) studied by CD, 1H-NMR and IR spectroscopies

The conformation of d(C-Br8G-C-G-C-Br8G) in aqueous solution was studied by CD and 1H-NMR spectroscopy and in condensed phase by IR spectroscopy. Whether in 0.1 M or 3 M NaCl solution or in film the only double helical structure adopted by brominated d(C-G)3 oligomer is the Z form. The IR spectrum of the film presents all the characteristic absorptions of the Z conformation and in particular is indicative of a syn conformation for the central guanosine as well as for the brominated one. Imino proton resonances of d(C-Br8G-C-G-C-Br8G) demonstrating the duplex formation were observed up to 60 degrees C. It is interesting to note that the significant highfield shifts of the dC H5" exocyclic sugar protons characteristic of the non exchangeable proton spectra of d(C-G)3 containing 5-methyl dC residues in the Z form were also detected in the proton spectrum of brominated oligomer. Whereas formation of the Z helix of methylated d(C-G)3 oligomers dependent on the salt concentration was found to occur via the preliminary formation of a B helix even in 4 M NaCl solution, the Z helix of d(C-Br8G-C-G-C-Br8G) is obtained directly from the coil form. However, IR data suggest that in the Z form of d(C-Br8G-C-G-C-Br8G), the overlapping of the base planes should be slightly different in comparison with the stacking observed in d(C-G)3 crystals. The kinetic data (activation energy and lifetime) of the Z helix-coil transition of brominated d(C-G)3 are compared to those of the B helix-coil transition observed for methylated d(C-G)3 in 0.1 M NaCl solution while the thermodynamic data of these two reactions (enthalpy and midpoint temperature) are slightly different.     

Berenil Complexation with a Nucleic Acid Triple Helix

Abstract

The interaction of berenii molecule, a minor groove binding drug, with T-A-T triple helix and A-T double helix was studied using circular dichroism spectroscopy and thermal denaturation. The triple helix was made by an oligonucleotide (dA)₁₂?x-(dT)₁₂?x-(dT)₁₂, where x is a hexaethylene glycol chain bridged between the 3′ phosphate of one strand and the 5′ phosphate of the following strand. This oligonucleotide is able to fold back on itself to form a very stable triplex. Circular dichroism spectroscopy demonstrates that berenil can bind to the triple helical structure. Spectral analysis shows that in the same ionic strength the drug bound to a double-stranded structure exhibits a conformation and an environment close to those observed in triple-stranded structure. The influence of the ionic strength on the interaction between the berenil molecule and the 36-mer is clearly demonstrated. We showed that when no NaCl salt is added in the buffer the triplex form of (dA)₁₂?x-(dT)₁2-x-(dT)₁₂ is stabilized by berenil whereas it is destabilized slightly by the dye when NaCl concentration is 1 M.     

B,Z conformations and mechanism of the Z-B-coil transitions of the self-complementary deoxy-hexanucleotide d(C-G-m5C-G-C-G) by 1H-NMR and CD spectroscopy

The helical structures of d(C-G-m5C-G-C-G) were studied in aqueous solution at various salt concentrations and temperatures by CD and 1H-NMR spectroscopy. At room temperature only the B form is observed in 0.1 M NaCl whereas the B and Z forms are simultaneously present in 1.8 M NaCl. At high salt concentration (4 M NaCl) the Z form is largely predominant (greater than 95%). The Z form proton resonances were assigned by using the polarisation transfer method (between B and Z at 1.8 M NaCl) and by proton-proton decoupling (at high salt concentration). The Z-B-Coil transitions were studied as a function of temperature with the 1.8 M NaCl solution. At high temperature (95 degrees C) only the coil form (S) is present. Below 55 degrees C the coil proportion is negligible, and the B-Z exchange is slow. The disappearance of the coil gives rise at first to the B form and on lowering the temperature the Z proportion increases to the detriment of the B form. Proton linewidth, relaxation and polarisation transfer studies confirm the conclusion in the previous report on d(m5C-G-C-G-m5C-G) (Tran-Dinh et al Biochemistry 1984 in the press) that Z exchanges only with B whereas the latter also exchanges with S,Z in equilibrium B in equilibrium S. The present data show that even at high salt concentration where only the Z form of d(C-G-m5C-G-C-G) is observed the Z-S transition also passes through the B form as an intermediate stage. The B-Z transition takes place when the Watson-Crick hydrogen bonds are firmly maintained and is greatly favoured when there are three hydrogen bonds between the base-pairs.     

B,Z Conformations and Mechanism of the Z-B-Coil Transitions of the Self-Complementary Deoxy-hexanucleotide d(C-G-m5C-G-C-G) by 1H-NMR and CD Spectroscopy

Abstract

The helical structures of d(C-G-m⁵C-G-C-G) were studied in aqueous solution at various salt concentrations and temperatures by CD and ¹H-NMR spectroscopy. At room temperature only the B form is observed in 0.1 M NaCl whereas the B and Z forms are simultaneously present in 1.8 M NaCl. At high salt concentration (4 M NaCl) the Z form is largely predominant (> 95%). The Z form proton resonances were assigned by using the polarisation transfer method (between B and Z at 1.8 M NaCl) and by proton-proton decoupling (at high salt concentration).

The Z-B-Coil transitions were studied as a function of temperature with the 1.8 M NaCl solution. At high temperature (95°C) only the coil form (S) is present. Below 55°C the coil proportion is negligible, and the B-Z exchange is slow. The disappearance of the coil gives rise at first to the B form and on lowering the temperature the Z proportion increases to the detriment of the B form. Proton linewidth, relaxation and polarisation transfer studies confirm the conclusion in the previous report on d(m⁵C-G-C-G-m⁵C-G) (Tran-Dinh et al Biochemistry 1984 in the press) that Z exchanges only with B whereas the latter also exchanges with S,Z ? B ? S. The present data show that even at high salt concentration where only the Z form of d(C-G-m⁵C-G-C-G) is observed the Z-S transition also passes through the B form as an intermediate stage. The B-Z transition takes place when the Watson-Crick hydrogen bonds are firmly maintained and is greatly favoured when there are three hydrogen bonds between the base-pairs.     

Influence of dA X dT and d(2aminoA) X dT base pairs on the B in equilibrium Z transition of DNA fragments. 1H-NMR study of d(C-G-C-A-m5C-G-T-G-m5C-G), d(m5C-G-C-A-m5C-G-T-G-C-G) and d(C-2aminoA-C-G-T-G)

The Helical structures of d(C-G-C-A-m5C-G-T-G-m5C-G), d(m5C-G-C-A-m5C-G-T-G-C-G) and d(C-2aminoA-C-G-T-G) were studied in aqueous solution at various salt concentrations and temperatures by 1H-NMR spectroscopy. In 0.1 M NaCl solution only the B form was evidenced for these DNA fragments whereas in 4 M NaCl both B and Z forms, in slow exchange on the NMR time scale, were observed. Under these conditions the Z form accounted for less than 60% of the decamer conformation; conversely d(C-G)3 hexamers containing methylated cytidines were predominantly in the Z form (greater than 90%) [Tran-Dinh et al. (1984) Biochemistry 23, 1362; Cavaillès et al. (1984) J. Biomol. Struct. Dyn. 1, 1347-1371]. On the other hand, d(C-2aminoA-C-G-T-G) in which the d(2aminoA) X dT base pair forms three hydrogen bonds, was found to adopt the Z conformation in 4M NaCl solution which was not the case for d(C-A-C-G-T-G) (unpublished results). The present study shows that the B in equilibrium Z transition in solution is highly sequence-dependent and that correlation exists between the stability of the duplexes (essentially governed by the number of hydrogen bonds between complementary bases) and their ability to adopt the Z conformation.     

Conformational peculiarities of polynucleotides with a nonrandom base sequence according to the 1H----3H exchange rate in C8H groups of purinic residues

We have determined the 1H----3H exchange rate constants between water and C8H groups of purinic residues of alternating polynucleotides poly(dA-dT).poly(dA-dT), poly(dG-dC).poly(dG-dC) and poly(dA-dC).poly(dG-dT) as well as homopolynucleotides poly(dA).poly(dT) and poly(dG).poly(dC) in aqueous solutions with high-salt concentrations (3 M NaCl and 4-6 M CsF), in water-ethanol (60%) solution and in 0.15 M NaCl at 25 degrees C. The rate constants for adenine (kA) and guanine (kG) of polynucleotides were compared with corresponding constants for E. coli DNA. dGMP nd dAMP at the same conditions. The relation between exchange rates and conformations of polynucleotides permits the study of their conformational peculiarities in solution. Of three alternating polynucleotides examined in 0.15 M NaCl the exchange retardation was observed only for poly(dA-dT).poly(dA-dT) as compared with that in B-DNA, which is in good agreement with the B-alternating "wrinkled" DNA model. The conformations of poly(dG-dC).poly(dG-dC) and poly(dA-dC).poly(dG-dT), according to the exchange data obtained are within the B form. For homopolynucleotides in 0.15 M NaCl, the KA value for poly(dA).poly(dT) is nearly the same as kA for B-DNA, which indicates the similarity of their conformations, whereas the kG value for poly(dG).poly(dC) is 1.7-fold lower in comparison with the kG value in B-DNA. This seems to be connected with the existence of B = A conformation equilibrium for poly(dG).poly(dC) in solution. The increase of NaCl concentration to 3 M results in a B----Z transition in the case of poly(dG-dC).poly(dG-dC) and in the shift of B = A equilibrium towards the A-form in the case of poly(dG).poly(dC) as is evidenced by alterations of their KG values. Poly(dA-dT).poly(dA-dT) in 6 M CsF and poly(dA-dC).poly(dG-dT) in 4.3 M CsF maintain their inherent conformations in 0.15 M NaCl in spite of the fact that they are characterised by the "X-type" CD-spectrum at these conditions. According to the exchange data the conformation of poly(dA).poly(dT) in 6 M CsF corresponds to the "heteronomous" DNA model or some other structure with lower accessibility of C8H groups of adenylic residues.     

Salt dependence of DNA structural stabilities in solution. Theoretical predictions versus experiments

The predictions of currently available theories for treating DNA-diffuse ionic cloud free energy contributions to conformational stability have been tested against experimental data for salt induced B-Z and B-A transitions. The theories considered are (i) Manning's counterion condensation approach (CC), (ii) the idealized Poisson-Boltzmann approximation (PB), and (iii) the potentials of mean force (PMF) approach proposed by Soumpasis. As far as we can judge from comparison with the set of experimental data currently available, it is found that only the latter theory yields satisfactory quantitative results for the dependence of the B-Z and B-A relative stabilities on monovalent salt concentration. The correct application of the PB and CC theories does not yield very low salt Z-B transitions, in contradiction to earlier assertions. At low salt concentrations the PB theory is qualitatively correct in predicting that the B form is electrostatically more favorable than both the A and Z forms, whereas the CC theory is qualitatively wrong predicting that Z-DNA is more stable than both B and A DNA.     

Conformational Peculiarities of Polynucleotides with a Nonrandom Base Sequence According to the 1H→ 3H Exchange Rate in C8H Groups of Purinic Residues

Abstract

We have determined the ¹H→³H exchange rate constants between water and C8H groups of purinic residues of alternating polynucleotides poly(dA-dT)·poly(dA-dT), poly(dG-dC)·poly(dG- dC) and poly(dA-dC)·poly(dG-dT) as well as homopolynucleotides poly(dA)·poly(dT) and poly(dG)·poly(dC) in aqueous solutions with high-salt concentrations (3 M NaCl and 4–6 M CsF), in water-ethanol (60%) solution and in 0.15 M NaCl at 25°C. The rate constants for adenine (k_A) and guanine (k_G) of polynucleotides were compared with corresponding constants for E.coli DNA, dGMP nd dAMP at the same conditions. The relation between exchange rates and conformations of polynucleotides permits the study of their conformational peculiarities in solution.

Of three alternating polynucleotides examined in 0.15 M NaCl the exchange retardation was observed only for poly(dA-dT)·poly(dA-dT) as compared with that in B-DNA, which is in good agreement with the B-alternating “wrinkled” DNA model. The conformations of poly(dG-dC)·poly(dG-dC) and poly(dA-dC)·poly(dG-dT), according to the exchange data obtained, are within the B form. For homopolynucleotides in 0.15 M NaCl, the k_A value for poly(dA)·poly(dT) is nearly the same as k_A for B-DNA, which indicates the similarity of their conformations, whereas the k_G value for poly(dG)·poly(dC) is 1.7-fold lower in comparison with the k_G value in B-DNA. This seems to be connected with the existence of B? A conformation equilibrium for poly(dG)·poly(dC) in solution.

The increase of NaCl concentration to 3 M results in a B→Z transition in the case of poly(dG-dC)·poly(dG-dC) and in the shift of B?A equilibrium towards the A-form in the case of poly(dG)·poly(dC), as is evidenced by alterations of their K_G values. Poly(dA-dT)·poly(dA-dT) in 6 M CsF and poly(dA-dC)·poly(dG-dT) in 4.3 M CsF maintain their inherent conformations in 0.15 M NaCl in spite of the fact that they are characterised by the “X-type” CD-spectrum at these conditions. According to the exchange data the conformation of poly(dA)·poly(dT) in 6 M CsF corresponds to the “heteronomous” DNA model or some other structure with lower accessibility of C8H groups of adenylic residues.     

Triple-helix formation by an oligonucleotide containing one (dA)12 and two (dT)12 sequences bridged by two hexaethylene glycol chains.

The triple-helix formation by the oligonucleotide (dA)12-x-(dT)12-x-(dT)12, where x is a hexaethylene glycol group, was investigated by thermal denaturation analysis and circular dichroism spectroscopy. Thermal denaturation analysis showed that this single-stranded oligonucleotide is able to fold back on itself twice to give a triple helix at low temperature. Upon an increase in the temperature, two cooperative transitions were observed: formation of a double-stranded structure with a dangling x-(dT)12 extremity, then formation of a single-stranded coil structure. Due to the intramolecular character of the transition, the triplex is much more stable than that formed by the reference mixture (dA)12 + 2(dT)12. In 0.1 M NaCl, the triplex-to-coil transition occurred at about 30 degrees C whereas the duplex-to-coil was at about 60 degrees C. Upon an increase in the salt, the increase of temperature corresponding to the triplex-to-duplex transition was larger than that of the duplex-to-coil transition. MgCl2 showed higher efficiency than NaCl to promote triplex or duplex formation. The thermodynamic parameters delta H and delta S were determined at various ionic strengths for both transitions. Both the enthalpy change and entropy change associated with triplex-to-duplex transition (Hoogsteen base pairing) were smaller than those associated to the duplex-to-coil transition (Watson-Crick base pairing). When the ionic strength increased, the parameters -delta H and -delta S showed a very small decrease for the duplex-to-coil transition whereas a strong increase was observed with the triplex-to-duplex transition.(ABSTRACT TRUNCATED AT 250 WORDS)     

Z Helix-coil Transition of d(C-Br8G-C-G-C-Br8G) Studied by CD, 1H-NMR and IR Spectroscopies

Abstract

The conformation of díC-Bi⁸G-C-G-C-Br⁸G) in aqueous solution was studied by CD and ¹H-NMR spectroscopy and in condensed phase by IR spectroscopy. Whether in 0.1 M or 3 M NaCl solution or in film the only double helical structure adopted by brominated d(C-G)₃ oligomer is the Z form. The IR spectrum of the film presents all the characteristic absorptions of the Z conformation and in particular is indicative of a syn conformation for the central guanosine as well as for the brominated one. Imino proton resonances of diC-Bi⁸G-C- G-C-Br⁸G) demonstrating the duplex formation were observed up to 60°C. It is interesting to note that the significant highfield shifts of the dC H₅″ exocyclic sugar protons characteristic of the non exchangeable proton spectra of d(C-G)₃ containing 5-methyl dC residues in the Z form were also detected in the proton spectrum of brominated oligomer. Whereas formation of the Z helix of methylated d(C-G)₃ oligomers dependent on the salt concentration was found to occur via the preliminary formation of a B helix even in 4 M NaCl solution, the Z helix of d(C-Br⁸G-C-G-C-Br⁸G) is obtained directly from the coil form. However, IR data suggest that in the Z form of dlC-Bi⁸G-C-G-C-Bi⁸G), the overlapping of the base planes should be slightly different in comparison with the stacking observed in d(C-G)₃ crystals. The kinetic data (activation energy and lifetime) of the Z helix-coil transition of brominated d(C-G)₃ are compared to those of the B helix-coil transition observed for methylated d(C-G)₃ in 0.1 M NaCl solution while the thermodynamic data of these two reactions (enthalpy and midpoint temperature) are slightly different.     

1H NMR and circular dichroism studies of the B and Z conformations of the self-complementary deoxyhexanucleotide d(m5C-G-C-G-m5-C-G): mechanism of the Z-B-coil transitions

The double-helical conformations of d(m5-C-G-C-G-m5-C-G) in aqueous solution were studied by circular dichroism and 1H NMR spectroscopy. In 0.1 M NaCl, only the B form is detected whereas the Z form is strongly predominant in 3 M NaCl. In the presence of 2 M NaCl, two resonance signals corresponding to the B and Z duplexes were observed for each proton below 50 degrees C, indicating a slow exchange between B and Z. However, the B-Z exchange becomes intermediate or fast in the 55-80 degrees C temperature interval. By contrast the exchange between B helix and single-stranded (or coil) forms is much faster for the same temperature conditions. The Z form is only detectable when the coil form is practically absent. With decreasing temperature the B form decreases in favor of the Z form. From proton line-width measurements under various experimental conditions, it was also shown that Z exchanges only with B, while the latter also exchanges with the single-stranded form (S): Z in equilibrium B in equilibrium S. The enthalpy value is about 8 +/- 1 kcal/mol for the B-Z transition and about 40 +/- 2 kcal/mol for the B-S dissociation (2 M NaCl solution). The activation energy is about 47 +/- 2 kcal/mol for the Z----B and 39 +/- 2 kcal/mol for the B----Z reaction. Very good agreement between the experimental results and computed data (based on the above kinetic reaction model) was found for the B, Z, and coil proportions. The B-Z transition of methylated d(C-G)n oligomers is only possible when the Watson-Crick hydrogen bonds between the CG base pairs are firmly maintained; otherwise, the transformation from B to Z would not occur, and B-S dissociation would take place instead.     

Relative stabilities and transitions of DNA conformations in 1:1 electrolytes: a theoretical study

We use a recently developed formalism (1) to calculate the salt dependent part of the free energy determining DNA conformational stability in 1:1 electrolytes. The conformations studied are the A, B, C and alternating-B right-handed forms and the ZI, ZII left-handed forms of DNA. In the case of the B-ZI transition of d(G-C).d(G-C) helices in NaCl solution, the free energy contribution considered suffices to describe the transition in a quantitative manner. The theory also predicts the occurrence of salt-induced B-A transitions which have been recently observed with poly[d(n2 A-T)] and poly[d(G-C)]. In other cases, additional terms in the free energy balance, particularly due to hydration effects, must be at least as important as salt effects in determining conformational stability and structural transitions in solution. If diffuse ionic cloud electrostatic effects alone would dominate in all cases, the relative helical stabilities at 0.2 M monovalent salt would decrease in the order C greater than B greater than A greater than ZII greater than ZI greater than alternating-B. At high salt concentrations (2.0 M-5.0 M), the order would be alternating-B greater than ZI greater than A greater than ZII greater than B greater than C.     

Relative Stabilities and Transitions of DNA Conformations in 1:1 Electrolytes: A Theoretical Study

Abstract

We use a recently developed formalism (1) to calculate the salt dependent part of the free energy determining DNA conformational stability in 1:1 electrolytes. The conformations studied are the A,B,C and alternating-B right-handed forms and the Z₁Z_II left-handed forms of DNA. In the case of the B-Z₁ transition of d(G-C) · d(G-C) helices in NaCl solution, the free energy contribution considered suffices to describe the transition in a quantitative manner. The theory also predicts the occurrence of salt-induced B-A transitions which have been recently observed with poly[d(n²A-T)| and poly[d(G-C)|. In other cases, additional terms in the free energy balance, particularly due to hydration effects, must be at least as important as salt effects in determining conformational stability and structural transitions in solution. If diffuse ionic cloud electrostatic effects alone would dominate in all cases, the relative helical stabilities at 0.2 M monovalent salt would decrease in the order C > B > A > Z_II > Z₁ > alternating-B. At high salt concentrations (2.0 M - 5.0 M), the order would be alternating-B > Z, > A > Z_II > B > C.     

Stabilization of triple-stranded oligonucleotide complexes: use of probes containing alternating phosphodiester and stereo-uniform cationic phosphoramidate linkages.

Pyrimidine oligonucleotides containing alternating anionic and stereo-uniform cationic N-(dimethylamino-propyl)phosphoramidate linkages [e.g. d(T+T-)7T, d(T+T-)2(T+C-)5T and (U'+U'-)7dT, where U' is 2'-O-methyluridine)] are shown to bind to complementary double-stranded DNA segments in 0.1 M NaCl at pH 7 to form triple-stranded complexes with the pyrimidine.purine.pyrimidine motif. For each of the sequences investigated, one stereoisomer bound with higher affinity, and the other stereoisomer with lower affinity, than the corresponding all-phosphodiester oligonucleotide. The stereoisomer of d(T+T-)7T that interacted weakly with a dT.dA target in 0.1 M NaCl formed a novel dA.dA.dT triple-stranded complex with poly(dA) or d(Al5C4A15) in 1 M NaCl; in contrast, the stereoisomer that bound strongly to the dT.dA target failed to form a dA.dA.dT triple-stranded complex.     

Theoretical studies of the electrostatic stability of A,B, C,and Z-DNA conformers as a function of monovalent ion concentration and ion type

Theoretical calculations using a two-state model of counterion phosphate interactions have been performed in order to determine the electrostatic stability of DNA in various ionic environments. Comparison of the stabilities of different conformations leads to results consistent with the B→Z transitions observed in high-salt environments and suggest that at very low ionic strnegths the left-handed Z(II) form is an electrostatically preferred conformation. An ion-type dependence of the high-salt B→Z transition midpoint is predicted. Calculations of the energies of the A and C conformations are also discussed in relation to experimentally observed transitions.     

The length of a junction between the B and Z conformations in DNA is three base pairs or less

Recently it has been suggested that double-helical complexes formed between the DNA sequences (CG)n(A)m and their conjugates, (T)m(CG)n, would be candidates for the formation of a B-Z junction in aqueous solution at high salt concentrations [Peticolas et al. (1988) Proc. Natl. Acad. Sci. U.S.A. 85, 2579-2583]. The junction was predicted to occur between a B-type helix in the d(A)m.d(T)m section and a Z-type helix in the self-complementary (CG)n.(CG)n sequence. In this paper we report Raman experiments on the deoxyoligonucleotides d(CGCGCGCGCGCGAAAAA) and d(CGCGCGAAAAA) and their complements. It is found the latter compound cannot be induced into the Z form in saturated salt solution but that the former sequence goes into a B-Z junction at 5.5 M salt. From a comparison of the relative intensity of the Raman conformational marker bands for B and Z DNA for both the A-T and C-G base pairs, it is shown that in 5.5 M NaCl solution none of the A-T base pairs are in the Z form, but nine of the C-G base pairs are in the Z form. The remaining three C-G base pairs are either in the junction or in the B form. Thus, the junction is formed from three or less C-G base pairs. If the solution is made 95 microM with NiCl2, then the entire duplex goes into the Z form and the Raman bands of the adenine are completely changed into those of the Z form.(ABSTRACT TRUNCATED AT 250 WORDS)     

Salt Dependence of DNA Structural Stabilities in Solution. Theoretical Predictions Versus Experiments

Abstract

The predictions of currently available theories for treating DNA-diffuse ionic cloud free energy contributions to conformational stability have been tested against experimental data for salt induced B-Z and B-A transitions. The theories considered are (i) Manning's counterion condensation approach (CC), (ii) the idealized Poisson-Boltzmann approximation (PB), and (iii) the potentials of mean force (PMF) approach proposed by Soumpasis. As far as we can judge from comparison with the set of experimental data currently available, it is found that only the latter theory yields satisfactory quantitative results for the dependence of the B-Z and B-A relative stabilities on monovalent salt concentration. The correct application of the PB and CC theories does not yield very low salt Z-B transitions, in contradiction to earlier assertions. At low salt concentrations the PB theory is qualitatively correct in predicting that the B form is electrostatically more favorable than both the A and B forms, whereas the CC theory is qualitatively wrong predicting that Z-DNA is more stable than both B and A DNA.     

The thermodynamic contribution of the 5-methyl group of thymine in the two- and three-stranded complexes formed by poly(dU) and poly(dT) with poly(dA)

To assess the thermodynamic contribution of the 5-methyl group of thymine, we have studied the two-stranded helical complexes poly(dA).poly(dU) and poly(dA).poly(dT) and the three-stranded complexes--poly(dA).2poly(dU), poly(dA).poly(dT).poly(dU) and poly(dA).2poly(dT)--by differential scanning calorimetry, and uv optical melting experiments. The thermodynamic quantities associated with the 3 --> 2, 2 --> 1, and 3 --> 1 melting transitions are found to vary with salt concentration and temperature in a more complex manner than commonly believed. The transition temperatures, T(m), are generally not linear in the logarithm of concentration or activity of NaCl. The change in enthalpy and in entropy upon melting varies with salt concentration and temperature, and a change in heat capacity accompanies each transition. The poly(dA).2poly(dU) triple helix is markedly different from poly(dA).2poly(dT) in both its CD spectrum and thermodynamic behavior, while the poly(dA).poly(dT).poly(dU) triple helix resembles poly(dA).2poly(dT) in these properties. In comparing poly(dA).2poly(dT) with either the poly(dA).poly(dT).poly(dU) or the poly(dA).2poly(dU) triplexes, the substitution of thymine for uracil in the third strand results in an enhancement of stability against the 3 --> 2 dissociation of deltadeltaG degrees = -135 +/- 85 cal (mol A)(-1) at 37 degrees C. This represents a doubling of the absolute stability toward dissociation compared to the triplexes with poly(dU) as the third strand. The poly (dA).poly (dT) duplex is more stable than poly(dA).poly(dU) by deltadeltaG degrees = -350 +/- 60 cal (mol base pair)(-1) at 37 degrees C. Poly(dA).poly(dT) has 50% greater stability than poly(dA).poly(dU) as a result of the dT for dU substitution in the duplex.     

Sequence dependent effects in methylphosphonate deoxyribonucleotide double and triple helical complexes.

Deoxyribooligonucleotides containing 19 repeating bases of A, T or U were prepared with normal phosphodiester (dA19, dT19, dU19) or methylphosphonate (dA*19, dT*19, dU*19) linkages. Complexes of these strands have been investigated at 1:1 and 1:2 molar ratios (purine:pyrimidine) by thermal melting and gel electrophoresis. There are dramatic sequence dependent differences in stabilities of complexes containing methylphosphonate strands. Duplexes of dA*19 with dT19 or dU19 have sharp melting curves, increased Tm values, and slopes of Tm versus log (sodium ion activity) plots reduced by about one half relative to their unmodified 'parent' duplexes. Duplexes of dA19 with either dT*19 or dU*19, however, have broader melting curves, reduced Tm values at most salt concentrations and slopes of less than one tenth the values for the unmodified duplexes. Duplex stabilization due to reduced phosphate charge repulsion is offset in the pyrimidine methylphosphonate complexes by steric and other substituent effects. Triple helical complexes with dA19 + 2dT19 and dA19 + 2dU19, which can be detected by biphasic melting curves and gel electrophoresis, are stable at increased Na+ or Mg+2 concentrations. Surprisingly, however, no triple helix forms, even at very high salt concentrations, when any normal strand(s) is replaced by a methylphosphonate strand. Since triple helical complexes with methylphosphonates have been reported for shorter oligomers, inhibition with larger oligomers may vary due to their length and extent of substitution.     

Conformation and reactivity of DNA in the complex with protein. IV. Circular dichroism of poly-L-histidine model complexes with DNA polymers and specificity of the interaction.

The CD study of the DNA-poly-L-histidine complex at high degree of protonation revealed that complex formation is already observable at 2 M NaCl. The influence of salt together with 5 M urea suggests that in addition to electrostatic interactions probably hydrogen bonding may favour specific complexes. Affinity of protonated histidines to AT-rich regions is strongly supported by the complexes formed with (dA.dT)-containing polymers. The psi-type structure occurs with poly(dA-dT)-poly(dA-dT) while poly(dA)-poly(dT) is restricted to form a similar psi-state on interaction with highly protonated poly-L-histidine. Differences in the helix winding properties due to variation in the sequence is suggested as a possible factor in the formation of the psi-type complexes. The mechanism of interaction including hydrogen bonding of histidine side-chains with an AT pair at high degree of protonation and with GC-regions at lower degree of protonation in the polypeptide structure is discussed.