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.     

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.     

The Zβ domain of human DAI binds to Z-DNA via a novel B-Z transition pathway

The human DNA-dependent activator of IFN-regulatory factor (DAI) protein, which activates the innate immune response in response to DNA, contains two tandem Z-DNA binding domains (Zα and Zβ) at the NH(2) terminus. The hZβ(DAI) structure is similar to other Z-DNA binding proteins, although it demonstrates an unusual Z-DNA recognition. We performed NMR experiments on complexes of hZβ(DAI) with DNA duplex, d(CGCGCG)(2), at a variety of protein-to-DNA molar ratios. The results suggest that hZβ(DAI) binds to Z-DNA via an active-di B-Z transition mechanism, where two hZβ(DAI) proteins bind to B-DNA to form the hZβ(DAI)-B-DNA complex; the B-DNA is subsequently converted to left-handed Z-DNA. This novel mechanism of DNA binding and B-Z conversion is distinct from Z-DNA binding of the human ADAR1 protein.     

Interaction of the Zalpha domain of human ADAR1 with a negatively supercoiled plasmid visualized by atomic force microscopy

Interest to the left-handed DNA conformation has been recently boosted by the findings that a number of proteins contain the Zα domain, which has been shown to specifically recognize Z-DNA. The biological function of Zα is presently unknown, but it has been suggested that it may specifically direct protein regions of Z-DNA induced by negative supercoiling in actively transcribing genes. Many studies, including a crystal structure in complex with Z-DNA, have focused on the human ADAR1 Zα domain in isolation. We have hypothesized that the recognition of a Z-DNA sequence by the Zα_ADAR1 domain is context specific, occurring under energetic conditions, which favor Z-DNA formation. To test this hypothesis, we have applied atomic force microscopy to image Zα_ADAR1 complexed with supercoiled plasmid DNAs. We have demonstrated that the Zα_ADAR1 binds specifically to Z-DNA and preferentially to d(CG)_n inserts, which require less energy for Z-DNA induction compared to other sequences. A notable finding is that site-specific Zα binding to d(GC)₁₃ or d(GC)₂C(GC)₁₀ inserts is observed when DNA supercoiling is insufficient to induce Z-DNA formation. These results indicate that Zα_ADAR1 binding facilities the B-to-Z transition and provides additional support to the model that Z-DNA binding proteins may regulate biological processes through structure-specific recognition.     

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.     

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.     

Stabilization of Z-DNA by polyarginine near physiological ionic strength.

The identification of left handed or Z-DNA in solutions of poly d(GC) in high salt suggests that left handed DNA may exist in biological systems if stabilized at lower ionic strength. In the present study we show that binding of polyarginine to the Z form of poly d(GC) results in a protein-Z-DNA complex stable near physiological ionic strength. The percentage of Z-DNA in the low salt polyarginine-poly d(GC) complex was measured from the DNA circular dichroism spectrum. The ratio of Z to B-DNA is a linear function of polyarginine concentration and is sensitive to proteolytic digestion by trypsin. These results suggest that arginine-rich proteins may stabilize Z-DNA in vivo.     

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 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.     

During B-Z Transition There is No Large Scale Breakage of Watson-Crick Base Pairs A Direct Demonstration Using 500 MHz 1H NMR Spectroscopy

Abstract

Monitoring of the Watson-Crick GNH1 proton in poly(dG-dC)-poly(dG-dC) at 500 MHz in 90% H₂0:10% D₂o at 30° C as a function of NaCl concentration (1.5 to 3.6 M), demonstrates that the bases retain Watson-Crick pairing throughout the transition. This observation unequivocally demonstrates that during the B-Z transition there is no large scale and detectable base pair opening and that macroscopically the phenomenon can be described as a direct helix to helix transition. We present frame by frame, an energetically sound stereodynamical trajectory for this transfiguration from right-handed B-DNA to left-handed Z-DNA.     

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.     

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.     

NMR study of hydrogen exchange during the B-Z transition of a DNA duplex induced by the Zα domains of yatapoxvirus E3L

The Yaba-like disease viruses (YLDV) are members of the Yatapoxvirus family and have double-stranded DNA genomes. The E3L protein, which is essential for pathogenesis in the vaccinia virus, consists of two domains: an N-terminal Z-DNA binding domain and a C-terminal RNA binding domain. The crystal structure of the E3L orthologue of YLDV (yabZα_E3L) bound to Z-DNA revealed that the overall structure of yabZα_E3L and its interaction with Z-DNA are very similar to those of hZα_ADAR1. Here we have performed NMR hydrogen exchange experiments on the complexes between yabZα_E3L and d(CGCGCG)₂ with a variety of protein-to-DNA molar ratios. This study revealed that yabZα_E3L could efficiently change the B-form helix of the d(CGCGCG)₂ to left-handed Z-DNA via the active-mono B-Z transition pathway like hZα_ADAR1.     

Stereochemical Effects of Methylphosphonate in B- and Z-DNA Helices: Variation in Hydrophobicity and Effective Widths of Grooves

Abstract

Stereochemical effects of methylphosphonate (MP) in B-DNA and Z-DNA duplexes are studied through molecular mechanics approach. Duplexes of different lengths, tetramers, hexamers, dodecamers are examined to assess the interstrand and intrastrand electrostatic effects due to MPs vis-a-vis phosphates. A variety of models which include duplexes with alternating S-MP and R-MP, alternating phosphate and MP and, duplexes posessing MPs in only one of the strands, are examined by considering both the S- and R-stereoisomers. Majority of the calculations are performed with CG sequences to delineate factors responsible for the stability of B- and Z-DNA as well as B × Z-DNA transition under nonionic conditions. The results show that both B- and Z-DNA duplexes are energetically favoured in the presence of MP due to overwhelming reduction in intrastrand as well as interstrand electrostatic repulsive interactions. The effect is distinct in oligomers longer than tetramers. Comparison of energetics of MP B- and Z-DNA duplexes suggests that an oligodeoxynucleotide such as d(CG)₆ with all phosphates replaced by MPs may favour equally both B- and Z-DNA conformations. The analysis further provides an estimate of electrostatic interactions, operating at the grooves under a variety of conditions. Several specific and localised effects due to S-MP and R-MP are seen at CG and GC steps in various B-DNA and Z-DNA models. S-MP in B- DNA reduces the effective major groove width by nearly 3 Å hence denying access to the functional groups of endonucleases thereby enhancing the resistance of MP-DNA to enzymatic digestion. Further, methyl groups of MP render the surface of the DNA helix to be significantly hydrophobic which may explain higher permeability of MP-DNA in membranes as well as its less soluble nature in aqueous media.     

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.     

Applying the stochastic difference equation to DNA conformational transitions: a study of B-Z and B-A DNA transitions

Despite the existence of numerous models to account for the B-Z DNA transition, experimenters have not yet arrived at a conclusive answer to the structural and dynamical features of the B-Z transition. By applying the stochastic difference equation to simulate the B-Z DNA transition, we have shown that the stretched intermediate model of the B-Z transition is more probable than other B-Z transition models such as the Harvey model. This is accomplished by comparing potential energy profiles of various B-Z DNA transition models and calculating relative probabilities based on the stochastic difference equation with respect to length (SDEL) formalism. The results garnered in this article allow for new approaches in determining the structural transition of B-DNA to Z-DNA experimentally. We have also simulated the B-A DNA transition using the stochastic difference equation. Unlike the B-Z DNA transition, the mechanism for the B-A DNA transition is well established. The variation in the pseudorotation angle during the transition is in good agreement with experimental results. Qualitative features of the simulated B-A transition also agree well with experimental data. The SDEL approach is thus a suitable numerical technique to compute long-time molecular dynamics trajectory for DNA molecules.     

Comparison of Different Approaches for Calculation of Polyelectrolyte Free Energy

Abstract

We consider the problem of the mean field (Poisson-Boltzmann) calculation of the electrostatic free energy for a strongly charged polyelectrolyte such as DNA in a salt solution. We compare two approaches to calculate the free energy: (i) direct one, starting from the statistical-mechanical expression for the electrostatic free energy and (ii) the polyion charge variation method. In the infinite dilution limit (in respect to polyion) and in excess salt (IDLES) the two approaches are fully equivalent. This is shown by straight forward algebra. We have performed specific calculations of the free energy difference for the case of B-Z transition in DNA as a function of ionic strength. As expected, the two approaches led to identical results. The ionic strength dependence of the B-to-Z free energy proves to be concaved up and as a result Z-DNA is stabilized at low ionic concentration as well as at high salt in full agreement with our previous results (M.D. Frank- Kamenetskii et al, J. Biomol. Struct. Dyn. 3, 35–42 (1985)). Our data quantitatively agree with the results of Soumpasis (D. M. Soumpasis, J. Biomol. Struct. Dyn. 6, 563–574 (1988)). However, his claim about the absence of the effect of stabilization of Z-DNA at low salt proves to be groundless, and the criticism of our earlier approach seems to be irrelevant.     

The inhibition of restriction endonucleases due to Z-DNA in negatively supercoiled plasmid.

Plasmid pGC20 containing the (dGC)9 insert in SmaI recognition site has been used to study the inhibition of cleavage by different restriction endonuclease due to Z-DNA formation in (dCG)10 sequence of the negatively supercoiled plasmid. Data obtained indicate the different sensitivity of restriction endonucleases to DNA conformational perturbations resulted from the Z-DNA formation. Therefore, the inhibition of DNA cleavage by a particular restriction endonuclease cannot serve as a criterion for the estimation of the length of B-Z junctions in circular supercoiled DNAs.