B-Z cooperativity and kinetics of poly(dG-m5dC) are controlled by an unfavorable B-Z interface energy

Thermodynamic and kinetic properties of the B-Z transition of poly(dG-m5dC) were investigated using polynucleotide samples ranging in length from 11000 to 300 base pairs. Van't Hoff enthalpy values increase with increasing polymer length for the B-Z transition in 0.35 mM MgCl2, 50 mM NaCl, 5 mM TRIS, pH 8. Rates of the B to Z transition increase with increasing polymer length for a jump of 0 to 3 mM MgCl2 in 50 mM NaCl, 5 mM TRIS, pH 8. The activation energy of the B to Z transition equals 7.9 +/- 0.3 kcal/mol and is length independent. Thermodynamic and kinetic data were fit to a model that simulates distribution of B- and Z-form tracts at the midpoint of B-Z equilibrium as a function of polymer length. A cooperative length of 1000 +/- 200 base pairs is estimated for the B-Z transition. A direct relationship between rates of the B to Z transition and the square of the van't Hoff enthalpy values of the B-Z transition reflects a dependence of kinetics and cooperativity upon the energy of the nucleation event. Faster B to Z transition rates with increasing polymer length can be explained by a mechanism rate limited by nucleation within the polymer instead of the ends.     

Effect of basic oligopeptides on the B-Z transition of poly(dG-dC). poly(dG-dC) in water-methanol solutions

The effect of basic oligopeptides (Lys-Ala-Ala)n (n = 1-5, 10) and (Lys-Leu-Ala)n (n = 1-4) on the B-Z transition of poly(dG-dC).poly(dG-dC) in water-methanol solutions was investigated using CD and uv spectroscopy. In the absence of peptides, the concentration of methanol at the midpoint of the B-Z transition is 64% at 25 degrees C. The transition is temperature dependent and the B conformation is preferred at higher temperatures. All peptides tested shift the midpoint of the B-Z transition to lower concentrations of methanol. For shorter peptides this effect increases with an increasing number of monomeric units, showing the importance of the number of positive charges in the peptide molecule. Al conditions of low methanol content, the trimer and tetramer of the (Lys-Leu-Ala)n series have a greater effect on the B-Z transition than the corresponding oligomers of the (Lys-Ala-Ala)n series. This indicates an important influence of the presence of hydrophobic groups in the peptide side chains on the binding. In the presence of peptides, the B-Z transition is also temperature dependent and the B conformation is preferred at higher temperatures. The addition of peptides results in an increase of the transition midpoint and of the transition width. These parameters were used for the calculation of the transition enthalpy delta HB-Z in 65% methanol, which is -1.15 +/- 0.25 kcal/base pair. Since the van't Hoff enthalpy delta HVH calculated from the temperature dependence of the B-Z transition in the absence of peptides is -130 kcal/mol, the length of the cooperative unit is about 110 base pairs. The results suggest that the mechanism of Z-DNA induction is similar but not identical with that involved in the action of metal cations in aqueous solution.     

A Model of the Strain-induced B-Z Transition

Abstract

The B-to-Z transition in supercoiled circular DNA is modeled as a strain-induced nonlinear excitation process. Using a model, in which DNA is regarded as a chain of units with a bistable energy function along the twisting coordinate together with a harmonic inter-unit interaction, we show that a Z region and the accompanying two B-Z junctions of finite width appear naturally as a solution of nonlinear equations, when the strain exceeds a critical value. We examine the B-Z transition behaviour as a function of twist under various situations. We also analyse available experimental results on B-Z transition in supercoiled plasmid with G-C insertions by this mechanistic model in order to estimate the magnitude of model parameters. The energy barrier of the B-Z transition is estimated to be of the order of 1 kcal/mole per base pair. The analysis shows that if the length of the insertion is less than a certain value, the entire insertion converts to Z form at a transition point, but if the insertion is much longer, the B-Z transition exhibits a different behavior, in which part of the insertion flips to Z form and the Z region expands linearly upon changing linking number.     

B-Z Transition of Synthetic Oligonucleotides Containing Non-Z Forming Elements

Abstract

Ten oligonucleotides of the length 8–12 base pairs have been synthesized, which contain, in addition to the obligatory sequences CG/CG, sequences not favorable for the transition to the Z conformation (AT pairs, GG/CC or AA/TT sequences). Conformational transitions of these oligonucleotides in high concentrations of NaClO₄ in the absence and in the presence of Ni²⁺ were investigated using CD spectroscopy.

The B-Z transition is affected by the length and sequence of the oligonucleotide. Increasing the NaC1O₄ concentration alone the transition of only one of the oligonucleotides studied, (CGCGCGTGC ACGCGCG)₂, can be induced. Other oligonucleotides remain in the B conformation or only partial transition to the Z conformation can be observed.

Most other oligonucleotides can be converted into the Z conformation at intermediate concentrations of NaC1O₄ (2.0?3.2 M) by an addition of Ni²⁺ ions. In some cases, however, Ni²⁺ can destabilize the double stranded structure of the sample. We have studied the effect of the presence of A.T pairs in the G.C containing oligonucleotides and the effect of the presence of pu-pu/pyr-pyr sequences. The presence of the latter sequences in the Z form implicates the formation of a Z-Z′ junction which makes the transition quite difficult. Despite the fact that some oligonucleotides contained several structural elements not favorable for the transition, we did not find any sequence which would completely block the ability of the oligonucleotide to adopt the Z conformation.     

Left-handed Z Form in Superhelical DNA: A Theoretical Study

Abstract

This is a comprehensive statistical mechanical treatment of the Z form formation in purine- pyrimidine stretches of different length inserted into superhelical DNA. The B-Z transition for short inserts is shown to follow the “all-or-none” principle. Over some critical value of the insert length n, the B-Z transition in the insert proceeds in two stages. The flipping of m base pairs into the Z form is followed by a gradual growth of the Z-form stretch until it occupies the whole insert. By fitting the theoretical transition curves to experimental ones the fundamental thermodynamic parameters of the B-Z transition have been determined: the B-Z junction energy Fj = 4–5kcal?mol^?1 and the free energy change ΔF_B-Z = 0.5–0.7 kcal?mol^?1 under standard salt conditions. Calculations show that the B-Z transition in short purine-pyrimidine inserts may be seriously affected by cruciform formation in the carrier DNA.     

The Energetics of the B-Z Transition in DNA

Abstract

The paper deals with the energetics of the transition to left-handed Z form in DNA with an arbitrary base sequence. There is a brief outline of the statistical-mechanical model of the B-Z transition allowing for three possible states of each base pair. The parameters of the model can be determined by comparing the theory with experimental data for the B-Z transition in inserts with given sequences in circular DNA The model contains six energy parameters, most of which have been determined before. In order to find the remaining parameters of the model and test its adequacy, a number of oligonucleotide sequences were synthesized and inserted into the pUC 19 plasmid. Two-dimensional gel electrophoresis was used to determine the superhelical density at which the inserts adopt the Z form. A statistical-mechanical treatment of these data yielded a complete set of six energy parameters for the B-Z transition. The theoretical assumption that the free energy of Z-form pairs does not depend on the type of adjacent pairs proved to be in agreement with the experimental data.     

The energetics of the B-Z transition in DNA

The paper deals with the energetics of the transition to left-handed Z form in DNA with an arbitrary base sequence. There is a brief outline of the statistical-mechanical model of the B-Z transition allowing for three possible states of each base pair. The parameters of the model can be determined by comparing the theory with experimental data for the B-Z transition in inserts with given sequences in circular DNA. The model contains six energy parameters, most of which have been determined before. In order to find the remaining parameters of the model and test its adequacy, a number of oligonucleotide sequences were synthesized and inserted into the pUC 19 plasmid. Two-dimensional gel electrophoresis was used to determine the superhelical density at which the inserts adopt the Z form. A statistical-mechanical treatment of these data yielded a complete set of six energy parameters for the B-Z transition. The theoretical assumption that the free energy of Z-form pairs does not depend on the type of adjacent pairs proved to be in agreement with the experimental data.     

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.     

Sequence effects on the relative thermodynamic stabilities of B-Z junction-forming DNA oligomeric duplexes

Circular dichroism (CD) and ultraviolet absorption techniques were employed in characterizing the sequence-dependent thermodynamic stabilities of B-Z junction-forming DNA duplexes. The Watson strand of the duplexes has the general sequence (5meC-G)4-NXYG-ACTG (where N = A or G and XY represents all permutations of pyrimidine bases). Duplexes were generated by mixing stoichiometric amounts of the complementary strands. Circular dichroism studies indicate that each duplex is fully right-handed at low salt (e.g., 115 mM Na+) but undergoes a salt-induced conformational transition to a structure that possesses both left- and right-handed conformations at high salt (4.5 M Na+), and hence a B-Z junction. Optical melting studies of the DNA duplexes at fixed DNA concentration with total Na+ concentration ranging from 15 mM to 5.0 M were determined. A nonlinear dependence of the melting temperature (Tm) on [Na+] was observed. Thermodynamic parameters at Na+ concentrations of 115 mM and 4.5 M with a wide range of DNA concentrations were determined from UV optical melting studies via construction of van't Hoff plots. A change of a single dinucleotide within these duplexes significantly affected the helix stabilities. The experimentally obtained free energies for the duplex to single-strand transitions were in close agreement with predicted values obtained from two different methods.     

A model of the strain-induced B-Z transition

The B-to-Z transition in supercoiled circular DNA is modeled as a strain-induced nonlinear excitation process. Using a model, in which DNA is regarded as a chain of units with a bistable energy function along the twisting coordinate together with a harmonic inter-unit interaction, we show that a Z region and the accompanying two B-Z junctions of finite width appear naturally as a solution of nonlinear equations, when the strain exceeds a critical value. We examine the B-Z transition behaviour as a function of twist under various situations. We also analyse available experimental results on B-Z transition in supercoiled plasmid with G-C insertions by this mechanistic model in order to estimate the magnitude of model parameters. The energy barrier of the B-Z transition is estimated to be of the order of 1 kcal/mole per base pair. The analysis shows that if the length of the insertion is less than a certain value, the entire insertion converts to Z form at a transition point, but if the insertion is much longer, the B-Z transition exhibits a different behavior, in which part of the insertion flips to Z form and the Z region expands linearly upon changing linking number.     

B-A and B-Z transitions in deoxyoligoduplexes containing 4- and 5- methylcytosine

Self-complementary oligodeoxynucleotides: GGACCCGGGTCC, GGA4mCCCGGGTCC, GGA5mCCCGGGTCC, CGCGCGCG, CG4mCGCGCG, CG5mCGCGCG were synthetized to study the contribution of methyl groups into the energetics of the three known cooperative transitions in DNA: helix-coil, B-A and B-Z With the use of circular dichroism and absorbtion methods the profiles of the above transitions were obtained by variation of temperature (helix-coil), trifluoroethanol fraction (B-A), NaCl and trifluorethanol contents (B-Z). On the basis of the transition widths and shifts of the transition points due to the methylations the energetics of the methyl groups was estimated. 5mC stabilizes the B form relatively the A form by 0.33 kcal/mol; while 4mC by 0.5 kcal/mol. In the B-Z transition 5 mC stabilizes the Z form by 0.28 kcal/mol relatively the B form; 4mC stabilizes also the Z form although by 0.14 kcal/mol only. Thus, these naturally occurring modifications could modulate substantially the ability of a DNA piece to shift into the A or Z form.     

Chemical Probing of the B-Z Transition in Negatively Supercoiled DNA

Abstract

An analysis of the B-to-Z transition as a function of supercoiling for a natural Z-DNA- forming sequence found in plasmid pBR322 is presented at nucleotide resolution. The analysis is based on reactivity to four chemical probes which exhibit hyperreactivity in the presence of Z-DNA: hydroxylamine, osmium tetroxide, diethyl pyrocarbonate and dimethyl sulfate. We find that the initial transition occurs largely within a 14 base pair region which is mostly alternating purines and pyrimidines. With increasing negative supercoiling, Z-DNA extends into flanking regions having less and less alternating character, first in one direction and then in the other. Evidence of B-Z junctions is seen at four sites bracketing these three adjacent regions. One of these Z-forming regions contains the non-alternating sequence CTCCT, suggesting that such sequences can form Z-DNA without great difficulty if they are adjacent to alternating sequences. A plasmid containing three copies of a 61 base pair fragment bearing the entire Z-forming region shows equal reactivity of all three copies at any given superhelical density, implying that they compete equally and independently for the torsional strain energy which promotes the B-Z transition, and are unaffected by adjacent sequences more than 20–30 base pairs away.     

Helix-coil dynamics of a Z-helix hairpin

The helix–coil transition of a Z-helix hairpin formed from d(C-G)₅T₄(C-G)₅ has been characterized by equilibrium melting and temperature jump experiments in 5M NaClO₄ and 10 mM Na₂HPO₄, pH 7.0. The melting curve can be represented by a simple all-or-none transition with a midpoint at 81.6 ± 0.4°C and an enthalpy change of 287 ± 15 kJ/mole. The temperature jump relaxation can be described by single exponentials at a reasonable accuracy. Amplitudes measured as a function of temperature provide equilibrium parameters consistent with those derived from equilibrium melting curves. The rate constants of Z-helix formation are found in the range from 1800 s^?1 at 70°C to 800 s^?1 at 90°C and are associated with an activation enthalpy of ?(50 ± 10) kJ/mole, whereas the rate constants of helix dissociation are found in the range from 200 s^?1 at 70°C to 4500 s^?1 at 90°C with an activation enthalpy +235 kJ/mole. These parameters are consistent with a requirement of 3–4 base pairs for helix nucleation. Apparently nucleation occurs in the Z-helix conformation, because a separate slow step corresponding to a B to Z transition has not been observed. In summary, the dynamics of the Z-helix–coil transition is very similar to that of previously investigated right-handed double helices.     

The B-Z transition in supercoiled DNA depends on sequence beyond nearest-neighbors.

In order to examine sequence-dependent structural effects in DNA, the ability of alternating purine-pyrimidine fragments to undergo a B-Z transition when cloned in a supercoiled plasmid was determined solely as a function of sequence, with base and nearest-neighbor composition held constant. Sequences of 22 GC and 2 AT base pairs were synthesized such that the AT base pairs varied between contiguous placement and separation by eight GC base pairs. Results show, surprisingly, that the ease of the B-Z transition varies with the position of the two AT base pairs, occurring at lower superhelical densities when AT base pairs are contiguous, and at higher torsional strain when the AT base pairs are moved further apart.     

Effects of 5 cytosine methylation on the B-Z transition in DNA restriction fragments and recombinant plasmids

Alternating (dC-dG)n regions in DNA restriction fragments and recombinant plasmids were methylated at the 5 position of the cytosine residues by the HhaI methylase. Methylation lowers the concentration of NaCl or MgCl2 necessary to cause the B-Z conformational transition in these sequences. Ionic strengths higher than physiological conditions are required to form the Z conformation when the methylated (dC-dG)n tract is contiguous with regions that do not form Z structures, in contrast to the results with the DNA polymer poly(m5dC-dG) . poly(m5dC-dG). In supercoiled plasmids containing (dC-dG)n sequences, methylation reduces the number of negative supercoils necessary to stabilize the Z conformation. Calculations of the observed free energy contributions of the B-Z junction and cytosine methylation suggest that two junctions offset the favorable effect of methylation on the Z conformation in (dC-dG)n sequences (about 29 base-pairs in length). Studies with individual methylated topoisomers demonstrate that increasing Na+ concentration up to approximately 0.2 M inhibits the formation of the Z conformation in the (m5dC-dG)n region of supercoiled plasmids. The results suggest that methylation may serve as a triggering mechanism for Z DNA formation in supercoiled DNAs.     

Allosteric conversion of Z DNA to an intercalated right-handed conformation by daunomycin

Absorbance and fluorescence methods were used to measure the binding of the anticancer drug daunomycin to poly (dGdC) under ionic conditions that initially favor the left-handed Z conformation of the polymer. Drug binding was cooperative under these conditions and may be fully accounted for by an allosteric model in which the drug binds preferentially (but not exclusively) to the right-handed B conformation and shifts the polymer from the Z to an intercalated right-handed conformation. Quantitative analysis of binding isotherms in terms of the allosteric model allowed for estimation of the equilibrium constants for the conversion of a base pair at a B-Z interface from the Z to the B conformation and for the formation of a base pair in the B conformation within a stretch of helix in the Z conformation. The free energy of the Z to B conversion of a base pair was calculated from this data and ranges from +0.03 to +0.3 kcal/mol over the NaCl range of 2.4-3.5 M. The free energy for the formation of a B-Z junction was nearly constant at +4.0 kcal/mol over the same range of NaCl concentrations. The salt dependence of the free energy of the Z to B transition indicates preferential Na+ binding to the Z form and that there is a net release of Na+ upon conversion of a base pair from the Z to the B conformation. The energetically unfavorable Z to B transition was found by this analysis to be driven by coupling to the energetically favorable interaction of daunomycin with B form DNA. In 3.5 M NaCl, for example, the free energy change for the overall reaction (Z DNA base pairs) + (daunomycin) in equilibrium with (right-handed complex) is -7.0 kcal/mol, nearly all of which is contributed by the binding of drug to B DNA. Analysis using the allosteric model also shows that the number of base pairs converted from the Z to the B conformation per bound drug molecule is salt dependent and provides evidence that drug molecules partition into regions of the polymer in the right-handed conformation.     

Methylation of cytosine in the 5-position alters the structural and energetic properties of the supercoil-induced Z-helix and of B-Z junctions

The structural and energetic consequences of cytosine methylation in the 5-position on the supercoil-dependent B-Z equilibrium in alternating dC-dG sequences cloned into recombinant plasmids were investigated. The helical parameters determined with the band shift method for right-handed [10.7 base pairs (bp)/turn] and left-handed (12.8 bp/turn) 5MedC-dG inserts were different from the helical repeat values for unmethylated dC-dG inserts (10.5 bp/turn in the right-handed and 11.5 bp/turn in the left-handed form). We analyzed the thermodynamic parameters delta GBZ (free energy difference per base pair between right-handed and left-handed helix structure), delta Gjx (free energy for formation of one B-Z junction), and b (helix unwinding at a junction region) for varying lengths of dC-dG inserts by two-dimensional gel electrophoresis and application of a statistical mechanics model. A comparison of plasmids fully methylated in vitro with HhaI methylase and their unmethylated counterparts revealed that delta Gjx is not significantly changed by cytosine methylation. However, this base modification results in an approximate 3-fold decrease of delta GBZ and an approximate 2-fold decrease of the unwinding b at B-Z junction regions. Analysis of a pair of related plasmids, each containing two dC-dG blocks, revealed qualitatively different transition behaviors. When the two dC-dG blocks were separated by 95 bp of a mixed sequence, they underwent independent B to Z transitions with separate nucleation events and junction formations. When the two blocks were separated by only a 4 bp GATC sequence, only one nucleation event was necessary, and the Z-helix spread across the nonalternating GATC region.(ABSTRACT TRUNCATED AT 250 WORDS)     

AAF linked to the guanine amino group: a B-Z junction.

Minimized conformational potential energy calculations have been performed for AAF linked to dCpdG at the guanine amino group. This is a model for the minor AAF adduct observed in DNA, whose conformational influence has been difficult to ascertain. A global minimum energy conformation was computed with torsion angles like those of the dCpdG residue of Z-DNA. This conformation was incorporated into a larger polymer model at a B-Z junction, with the carcinogen residing in the groove in the Z direction. Local minimum energy conformations of the B type were also computed. In addition, two minima were found with fluorenecytidine stacking. These results suggest that existing B-Z junctions may be vulnerable to modification by AAF at the guanine amino group, or that such junctions may be induced by the carcinogen if the base sequence is appropriate. Otherwise the carcinogen can be located in the minor groove of the B helix (5, 10, 11) or covalently intercalated (13-15).     

Conformational Transitions in Poly d(CGCGCGTTAATT)

Abstract

Conformational studies on poly d(CGCGCGTTAATT) in solution by circular dichroism spectroscopy are reported. The polynucleotide exhibits B conformation in sodium chloride solution and on addition of NiCl₂ a B-Z transition is observed. NiCl₂ titrations carried out in the presence of 5M NaCl show a midpoint of transition at 2.25 mM NiCl₂ and a complete (maximum conversion to Z form) transition at 16 mM NiCl₂. In 60% alcohol the polynucleotide remains in B conformation. The polynucleotide isomerizes into ψ and A conformations in the presence of spermidine and spermine respectively. The thermodynamic parameters calculated from the melting profiles using a two state model show that the polynucleotide is almost equally stable in its B and Z conformations.     

Left-handed Z form in superhelical DNA: a theoretical study

This is a comprehensive statistical mechanical treatment of the Z form formation in purinepyrimidine stretches of different length inserted into superhelical DNA. The B-Z transition for short inserts is shown to follow the "all-or-none" principle. Over some critical value of the insert length n, the B-Z transition in the insert proceeds in two stages. The flipping of m base pairs into the Z form is followed by a gradual growth of the Z-form stretch until it occupies the whole insert. By fitting the theoretical transition curves to experimental ones the fundamental thermodynamic parameters of the B-Z transition have been determined: the B-Z junction energy Fj = 4-5kcal.mol-1 and the free energy change delta FBZ = 0.5-7.0 kcal.mol-1 under standard salt conditions. Calculations show that the B-Z transition in short purinepyrimidine inserts may be seriously affected by cruciform formation in the carrier DNA.