Competing B-Z and helix-coil conformational transitions in supercoiled plasmid DNA.

The formation of melted regions from A + T-rich sequences and left-handed Z-DNA by alternating purine-pyrimidine sequences will both be facilitated by negative supercoiling, and thus if the sequences are present within the same plasmid molecule they will compete for the free energy of supercoiling. We have studied a series of plasmids that contain either (CG)8 or (TG)12 sequences in either G + C or A + T-rich contexts, by means of two-dimensional gel electrophoresis and chemical modification. We observe both B-Z and helix-coil transitions in all plasmids at elevated temperatures and low ionic strength. The plasmids fall into a number of different classes, in terms of the conformational behavior. As the superhelix density is increased, pCG8/vec ((CG)8 in G + C-rich context) undergoes an initial B-Z transition, followed by melting transitions in sequences remote from the (CG)8 sequence. The two transitions are coupled through the topology of the molecule but are otherwise independent. When the (CG)8 sequence was placed in an A + T-rich context (pCG8/col), the helix-coil transition was perturbed by the presence of the Z-DNA segment. Replacement of the (CG)8 tracts by (TG)12 sequences resulted in a further level of interaction between the transitions. Statistical mechanical modeling of the transitions suggested that at intermediate levels of negative supercoiling the Z-DNA formed by the (TG)12 sequence has a lowered probability due to the helix-coil transition in the A + T-rich sequences. These studies illustrate the complexities of competing conformational equilibria in supercoiled DNA molecules.     

Stochastic distribution of a short region of Z-DNA within a long repeated sequence in negatively supercoiled plasmids

We have analyzed, at nucleotide resolution, the progress of the B-to-Z transition as a function of superhelical density in a 2.2-kilobase plasmid containing the sequence d(C-A)31.d(T-G)31. The transition was monitored by means of reactivity to two chemical probes: diethyl pyrocarbonate, which is sensitive to the presence of Z-DNA, and hydroxylamine, which detects B-Z junctions. At a threshold negative superhelical density between about 0.048 and 0.056, hyper-reactivity to diethyl pyrocarbonate appears throughout the CA/TG repeat and remains as the superhelical density is further increased. However, there is no reactivity characteristic of B-Z junctions until the superhelical density reaches 0.084, when single cytosines at each end of the repeat become hyper-reactive to hydroxylamine. A two-dimensional gel analysis of this system by others (Haniford, D. B., and Pulleyblank, D. E. (1983) Nature 302, 632-634) indicates that only about half of the 62 base pairs of the CA/TG repeat undergo the initial transition at omega = 0.056. Our results indicate that this region of Z-DNA is free to exist anywhere along the CA/TG repeat and is probably constantly in motion. Well defined B-Z junctions are seen only when there is sufficient supercoiling to convert the entire CA/TG sequence to Z-DNA. The implications for possible B-Z transitions in chromosomal domains of different sizes are discussed.     

The IN-VIVO Occurrence of Z DNA

Abstract

The energetics of the B-Z transition of two different types of cloned alternating purine/pyrimidine DNA sequences have been analysed by a two dimensional electrophoretic technique. Since the transition between right handed and left handed forms of these polymers is detected by alterations of electrophoretic mobilities of topoisomers of the plasmid DNA molecules, the method is not dependent on Z-DNA binding ligands. The measurements reflect intrinsic properties of the DNA unperturbed by the free energy of binding such a ligand.

Direct evidence from the analysis of topoisomer distributions is presented which shows that d(GC)n.d(GC)n sequence elements within an E. coli plasmid will adopt a Z conformation in-vivo under conditions of blocked protein synthesis. Evidence for the in-vivo occurrence of Z-DNA was not detected in plasmid DNA isolated from bacterial cells growing in the absence of protein synthesis inhibitors.

A model is proposed for a function for the B-Z transition in ensuring the correct pairing of homologous chromosomes during meiosis.     

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.     

Left-handed Z-DNA and intramolecular triplex formation at the site of an unequal sister chromatid exchange

An unequal sister chromatid exchange (USCE) in the mouse myeloma cell line MPC-11 between 3' regions of the C gamma 2a and C gamma 2b heavy chain genes results in duplication of the C gamma 2a heavy chain gene and generation of a novel recombination joint. The USCE occurs between (TC)n tracts adjacent to alternating purine-pyrimidine tracts. We have investigated the capacity of both the donor regions and the recombinant product involved in this event to adopt left-handed Z-DNA and intramolecular triplexes. The results of chemical probing with diethylpyrocarbonate and osmium tetroxide at the base pair level demonstrate that under the influence of negative supercoiling the alternating purine-pyrimidine regions of these plasmids can adopt Z-DNA at neutral pH, and the oligopurine.oligopyrimidine (pur.pyr) regions of these regions can adopt intramolecular triplexes at low pH (less than or equal to pH 6.0). At intermediate pH values, mixtures of both structures are present. Increasing the negative superhelical density of the plasmid does not increase the amount of triplex present at neutral pH indicating that the presence of long Z-DNA segments adjacent to pur.pyr tract prevents intramolecular triplex formation. In summary, we conclude that the sequences involved in the USCE can form either an intramolecular triplex in the (TC)n tract or Z-DNA in the alternating purine-pyrimidine tract and that Z-DNA will predominate under physiological conditions. The presence of segments which adopt Z-DNA at a site of USCE suggests that formation of this structure may enhance recombination between adjacent pur.pyr tracts.     

Formation of Z-DNA in negatively supercoiled plasmids is sensitive to small changes in salt concentration within the physiological range.

Negative supercoiling of the plasmid pBR322 with or without an insert of (dG-dC)n induces the formation of Z-DNA as measured by the binding of antibodies specific for Z-DNA. Increasing the concentration of Na+ (or K+) is shown to inhibit the B to Z-DNA conversion. This may be due to the effect of the cation on the B-Z junction. Using the data for B to Z-DNA conversion of the (dG-dC)n inserts, we have estimated the free energy change per base pair as well as the energy of the B-Z junction. In pBR322, a 14-bp segment [CACGGGTGCGCATG] is believed to form Z-DNA at bacterial negative superhelical densities under salt conditions which are similar to those found in vivo.     

The in-vivo occurrence of Z DNA

The energetics of the B-Z transition of two different types of cloned alternating purine/pyrimidine DNA sequences have been analysed by a two dimensional electrophoretic technique. Since the transition between right handed and left handed forms of these polymers is detected by alterations of electrophoretic mobilities of topoisomers of the plasmid DNA molecules, the method is not dependent on Z-DNA binding ligands. The measurements reflect intrinsic properties of the DNA unperturbed by the free energy of binding such a ligand. Direct evidence from the analysis of topoisomer distributions is presented which shows that d(GC)n.d(GC)n sequence elements within an E. coli plasmid will adopt a Z conformation in-vivo under conditions of blocked protein synthesis. Evidence for the in-vivo occurrence of Z-DNA was not detected in plasmid DNA isolated from bacterial cells growing in the absence of protein synthesis inhibitors. A model is proposed for a function for the B-Z transition in ensuring the correct pairing of homologous chromosomes during meiosis.     

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.     

The Z-Z junction: the boundary between two out-of-phase Z-DNA regions

The boundary between two segments of Z-DNA that differ in the phase of their syn-anti alternation about the glycosidic bond is termed a Z-Z junction. Using chemical probes and two-dimensional gel electrophoresis, we examined a Z-Z junction consisting of the sequence d[(CG)8C(CG)8] inserted into a plasmid and used energy minimization techniques to devise a three-dimensional model that is consistent with the available data. We show that both alternating CG segments undergo the B-Z transition together to form a Z-Z junction. The junction is very compact, displaying a distinctive reactivity signature at the two base pairs at the junction. In particular, the 5' cytosine of the CC dinucleotide at the junction is hyperreactive toward hydroxylamine, and the two guanines of the GG dinucleotide on the complementary strand are less reactive toward diethyl pyrocarbonate than are the surrounding Z-DNA guanines. Statistical mechanical treatment of the 2-D gel data yields a delta G for forming the Z-Z junction equal to 3.5 kcal, significantly less than the cost of a B-Z junction and approximately equal to the cost of a base out of alternation (i.e., a Z-DNA pyrimidine in the syn conformation). The computer-generated model shows little distortion of the Z helix outside of the central two base pairs, and the energy of the structure and the steric accessibility of the reactive groups are consistent with the data.     

The zab domain of the human RNA editing enzyme ADAR1 recognizes Z-DNA when surrounded by B-DNA

The Zab domain of the editing enzyme ADAR1 binds tightly and specifically to Z-DNA stabilized by bromination or supercoiling. A stoichiometric amount of protein has been shown to convert a substrate of suitable sequence to the Z form, as demonstrated by a characteristic change in the CD spectrum of the DNA. Now we show that Zab can bind not only to isolated Z-forming d(CG)(n) sequences but also to d(CG)(n) embedded in B-DNA. The binding of Zab to such sequences results in a complex including Z-DNA, B-DNA, and two B-Z junctions. In this complex, the d(CG)(n) sequence, but not the flanking region, is in the Z conformation. The presence of Z-DNA was detected by cleavage with a Z-DNA specific nuclease, by undermethylation using Z-DNA sensitive SssI methylase, and by circular dichroism. It is possible that Zab binds to B-DNA with low affinity and flips any favorable sequence into Z-DNA, resulting in a high affinity complex. Alternatively, Zab may capture Z-DNA that exists transiently in solution. The binding of Zab to potential as well as established Z-DNA segments suggests that the range of biological substrates might be wider than previously thought.     

Unpaired bases in the B--Z junction of the supercoiled plasmid

The restriction analysis has been used to establish that O-beta-diethylaminoethylhydroxylamine (OHA) produces modification of unpaired cytidines in the polylinker region adjacent to the Z-insert (dG-dC)10. (dG-dC)10 in the negatively supercoiled plasmid pGC20. The length of the transition region between B- and Z-portions of DNA is not less than 36 bps. The reaction of OHA with the unpaired cytidines in the B-Z junction is a fixing one and produces no secondary despiralling of the neighboring regions. The reaction with DNA proceeds much slower than the one with monomers and single-strand polynucleotides. The structural nonuniformity has been observed, which is manifested in the alternating B and "non-B" form DNA in the B-Z junction. It is suggested that these junctions may contain nucleotide sequences which are stable to violation of the B structure during the change in superhelical density of DNA.     

A computer aided thermodynamic approach for predicting the formation of Z-DNA in naturally occurring sequences.

The ease with which a particular DNA segment adopts the left-handed Z-conformation depends largely on the sequence and on the degree of negative supercoiling to which it is subjected. We describe a computer program (Z-hunt) that is designed to search long sequences of naturally occurring DNA and retrieve those nucleotide combinations of up to 24 bp in length which show a strong propensity for Z-DNA formation. Incorporated into Z-hunt is a statistical mechanical model based on empirically determined energetic parameters for the B to Z transition accumulated to date. The Z-forming potential of a sequence is assessed by ranking its behavior as a function of negative superhelicity relative to the behavior of similar sized randomly generated nucleotide sequences assembled from over 80,000 combinations. The program makes it possible to compare directly the Z-forming potential of sequences with different base compositions and different sequence lengths. Using Z-hunt, we have analyzed the DNA sequences of the bacteriophage phi X174, plasmid pBR322, the animal virus SV40 and the replicative form of the eukaryotic adenovirus-2. The results are compared with those previously obtained by others from experiments designed to locate Z-DNA forming regions in these sequences using probes which show specificity for the left-handed DNA conformation.     

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.     

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)     

Characterization of genomic poly(dT-dG).poly(dC-dA) sequences: structure, organization, and conformation.

Hybridization studies suggest the abundant presence of poly(dT-dG).poly(dC-dA) (TG-element), a potential Z-DNA sequence, in eucaryotic genomes. We have isolated and characterized TG-elements from different locations in the human genome: from randomly isolated clones, associated with the actin gene family, and linked to another repeated element. The results indicate that the following features are typical of these TG-elements: the elements consist of 20 to 60 base pairs of (dT-dG)n.(dC-dA)n, the sequences characterized in our study were not flanked by direct or inverted repeats, the sequences are interspersed rather than in satellite blocks, the elements are not usually associated with other repeated elements, and some of the elements are found near coding sequences or in introns. Studies on the conformation of a genomic TG-element in a supercoiled plasmid indicate several distinct properties of the TG-element: it is in the Z-form only at low ionic strength, S1 nuclease recognizes its Z-form with a marked preference for one of the B-Z junctions, and the sensitive region extends for 20 base pairs near the B-Z junction. In contrast to the result with the supercoiled plasmid, S1 nuclease failed to recognize the TG-element in minichromosomes.     

Characteristics of Z-DNA helices formed by imperfect (purine-pyrimidine) sequences in plasmids

The capacities of three synthetic sequences to adopt left-handed helices were evaluated in recombinant plasmids. The sequences consisted of very short runs of (CG)n (n = 2-4) interspersed with runs of alternating A.T base pairs and/or with regions of non-alternating base pairs. The plasmids were studied by two-dimensional gel electrophoresis to determine the natures of the conformational transitions and their free energies of formation. These results coupled with analyses with chemical (diethyl pyrocarbonate, osmium tetroxide, and bromoacetaldehyde) and enzymatic (S1 nuclease, T7 gene 3 product, and MHhaI) probes indicated that the entire sequence was adopting a left-handed helix in each case. In one of these sequences, Z-DNA formation necessitated the retention of the anti conformation of one of the guanines in a region of non-alternation. In a sequence which contains out-of-phase regions of alternation, our results indicate the formation of a separate left-handed helix in the central (CG)2 region, thus forming two Z-Z junctions. In summary, we conclude that only very short regions of alternating CG are necessary to effect the B to Z transition and that this conformational change can be transmitted through non-alternating regions. A set of empirical rules governing the characteristics of the B to Z transition and the types of left-handed helices in supercoiled plasmids was derived from studies on a systematic series of 17 plasmids.     

Anti-Z-DNA antibody binding can stabilize Z-DNA in relaxed and linear plasmids under physiological conditions.

It is shown that anti-Z-DNA antibody binding can stabilize sequences of d(CG/GC)n and d(CA/GT)n in the Z-DNA conformation in a plasmid in the complete absence of supercoiling. This effect is quantitated by using antibody preparations of different affinities and varying concentrations. The d(CG/GC)n sequence can be stabilized under physiological conditions. This is the first demonstration that a region of Z-DNA can be stabilized by protein binding in a completely relaxed plasmid under physiological conditions. The antibody-Z-DNA complex in the relaxed plasmid is shown to be an equilibrium state and not a long-lived kinetic intermediate since specific binding of the antibody to linearized plasmids containing Z-forming sequences is observed.