A study of the B-A transition in DNA by gel electrophoresis

A procedure is developed for studying the B-A transition in DNA using gel electrophoresis. The starting point has been the idea that the junction between the A and B sections, which appear within the transition interval would increase the mobility of the DNA molecules. Indeed, the mobility of DNA in a gel is shown to increase in the middle of the B-A transition due to the formation of the largest possible number of boundaries between the B and A forms. The middle of the B-A transition in supercoiled DNA appears to be shifted against the middle of the transition in open circular (as well as linear) DNA by about 1.3% towards lower ethanol concentrations under the influence of the superhelical stress.     

A Study of DNA Melting in Concentrated Water-Alcohol Solutions

Abstract

The DNA melting profiles with high resolution have been studied for conditions corresponding to the B and A conformations of DNA in water-alcohol solutions. The melting profiles of the A-form and B-form DNA, their mean melting temperatures and melting range width were found to differ. DNA was shown to be heterogeneous in respect of the B-A transition, the GC-rich regions more readily converting into the A form than AT-rich ones. The presence of boundaries between the A and B sections within the transition zone did not smooth off the fine structure of melting profiles.     

CC/GG Contacts Facilitate the B to A Transition of DMA in Solution

Abstract

Self-complementary decadeoxynucleotides, CCGATATCGG, CCAGATCTGG, CCCTG- CAGGG, GGGGGCCCCC, were designed and synthesized to estimate the A-philic free energy of CC/GG contacts.

First, regions of temperature-stability of the double-stranded conformation were determined for each 10-mer. Then, circular dichroism spectra were recorded for the B-family forms at different temperatures, counter-ion concentrations and trifluoroethanol contents.

A cooperative change typical of the B-A transition is observed in the CD spectra at a trifluoroethanol content specific for each duplex. The positions of half-transition points were functions not only of the nucleotide sequence but of the duplex length as well: the B to A transitions were hindered in these 10-mers in comparison with a lengthy DNA. The B-phility value was estimated to be 3 kcal/mol of 10-mer.

The B-A transition point was shown to drop with an increase in the number of CC/GG contacts in a duplex. The designed 10-mers made it possible to estimate quantitatively the A- phility of CC/GG contact as compared with an average DNA: (F_A-F_B)CC=0.2 Kcal/mol, (F_A-F_B)DNA=0.7 Kcal/mol.     

Peculiarities of the B to A Transition of the λ Phage Regulatory Site OR3 and of Its Fragment

Abstract

Conformations of the synthetic deoxyoligonucleotide 17 base pairs long, which is an OR3 operator of λ phage, and of its 9-b.p. fragment were studied by the circular dichroism method (CD). The regions of stability of the double-stranded state were determined for these duplexes. A comparison of the CD spectra for these oligonucleotides with the CD for a lengthy DNA showed the conformation of these short DNA pieces to belong to the B-family.

A cooperative change in the CD spectra is observed in trifluoroethanol (TFE) solutions at a TFE concentration specific for each oligonucleotide, which is supposed to stem from a B to A transition. The length of the fragment was found to affect the ability for the B-A transition. The transition into the A form is hindered by 13% TFE for the short 9-nucleotide in comparison with the 17-nucleotide. We suggest that this is due to the B form stabilization by terminal base pairs (B-phility of the ends).     

Three-State Diagram for DNA

Abstract

Experimental phase diagrams (A form, B form, Coil) were built in the coordinates (a, alcohol fraction: T, temperature) for the natural DNAs and poly d(A-T). The main parameter of the B-A transition,—cooperativity length, v _o, was estimated by the slopes of the branches A-B, A-Coil, B-Coil in the vicinity of the triple point: v _o +AD0- 10-20 base pairs, which corresponds to the energy for the B/A junction of 1.2–1.8 kcal/mol.

We discovered two new effects which are due to the coexistence of the three different conformations in one polymeric molecule: an increase in the melting temperature above that for the ‘ideal’ triple point (i.e. for the case of the ideal phase transitions); a widening of the melting curve within the B-A transition range.

The physics of these phenomena is discussed.     

Modulation of the B-A transition of DNA by potential antitumor antibiotics. Influence of the base composition of DNA

The B-A transition of DNA in oriented films of DNA-drug complexes is more or less restricted as a consequence of drug binding as revealed by infrared linear dichroism. A fraction of DNA is irreversibly locked into the B form. This behavior is described by the number of DNA base pairs "frozen" in the B form by one drug molecule. This quantity is dependent on the DNA sequence the drug is attached to. In this paper, drug complexes of oriented films of NaDNA with a GC content of 42% from calf thymus and a GC-rich DNA from Micrococcus lysodeikticus were compared. The restriction of the B-A transition of DNA complexes with two intercalating antibiotics, aclacinomycin A and violamycin BI, is not severely influenced by the base composition of DNA. By contrast, the strong groove binding oligopeptide antibiotics netropsin and distamycin A are much less effective to restrict the B-A transition of GC-rich DNA than of AT-rich DNA. This finding is in agreement with previous results by other methods which support a model based upon a strong preference of AT clusters by these two non-intercalating drugs.     

Condensation prevails over B-A transition in the structure of DNA at low humidity

B-A transition and DNA condensation are processes regulated by base sequence and water activity. The constraints imposed by interhelical interactions in condensation compromise the observation of the mechanism by which B and A base-stacking modes influence the global state of the molecule. We used a single-molecule approach to prevent aggregation and mechanical force to control the intramolecular chain association involved in condensation. Force-extension experiments with optical tweezers revealed that DNA stretches as B-DNA under ethanol and spermine concentrations that favor the A-form. Moreover, we found no contour-length change compatible with a cooperative transition between the A and B forms within the intrinsic-force regime. Experiments performed at constant force in the entropic-force regime with magnetic tweezers similarly did not show a bistable contraction of the molecules that could be attributed to the B-A transition when the physiological buffer was replaced by a water-ethanol mixture. A total, stepwise collapse was found instead, which is characteristic of DNA condensation. Therefore, a low-humidity-induced change from the B- to the A-form base-stacking alone does not lead to a contour-length shortening. These results support a mechanism for the B-A transition in which low-humidity conditions locally change the base-stacking arrangement and globally induce DNA condensation, an effect that may eventually stabilize a molecular contour-length reduction.     

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.     

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.     

Fine structure in the B-A transition of native DNA

The B-A transition caused by high ethanol concentrations has been studied by the multi-dimensional spectrophotometer equipped with the computer-controlled microbullet. When ethanol concentration is increased, the CD signal at 270 nm of linearized ColEl DNA exhibits a biphasic transition; the first broad one and the second sharp one. The B-A transition of the ColEl DNA is much broader than that of alternative copolymers with shorter lengths. In addition, each PvuII restriction fragment of ColEl DNA has a different transition curve. Therefore the stability of the B-A transition varies along a long DNA molecule. The second transition is speculated to be caused by aggregation. When ethanol concentration is decreased, on the other hand, only a single transition shifted to lower ethanol concentration is observed. Thus the B-A transition curve has a hysteresis. A slow dissociation rate of the aggregation seems to cause the hysteresis.     

A study of DNA melting in concentrated water-alcohol solutions

The DNA melting profiles with high resolution have been studied for conditions corresponding to the B and A conformations of DNA in water-alcohol solutions. The melting profiles of the A-form and B-form DNA, their mean melting temperatures and melting range width were found to differ. DNA was shown to be heterogeneous in respect of the B-A transition, the GC-rich regions more readily converting into the A form than AT-rich ones. The presence of boundaries between the A and B sections within the transition zone did not smooth off the fine structure of melting profiles.     

Mechanochemical study of NaDNA and NaDNA-netropsin fibers in ethanol-water and trifluoroethanol-water solutions.

Highly oriented calf-thymus NaDNA fibers, prepared by a wet-spinning method, were complexed with netropsin in ethanol-water and trifluoroethanol (TFE)-water solutions. The relative fiber length, L/L0, was measured at room temperature as a function of ethanol or TFE concentration to obtain information on the B-A conformational transition. The B-A transition point and transition cooperativity of the fibers were calculated. The binding of netropsin to NaDNA fibers was found to stabilize B form and to displace the B-A transition to higher ethanol concentration, as indicated by its elongational effect on the fiber bundles. An increased salt concentration was found to reduce netropsin binding. In netropsin-free ethanol solution, the dissociation of bound netropsin from the DNA fibers was observable. Pure B-NaDNA fibers were found to be more stable in TFE solution than in ethanol solution. This was interpreted as being due to a different steric factor and a larger polarity of TFE compared with ethanol, resulting in its smaller capacity to reduce the water activity and dielectric constant of the medium in the immediate vicinity of DNA fibers. Therefore, the effect of netropsin binding on the B-A transition of NaDNA fibers became less obvious in TFE solution. In another series of experiments, L/L0 was measured as a function of temperature to obtain information on the helix-coil transition, or melting, as well as the B-A transition of NaDNA and NaDNA-netropsin fibers. The melting temperature and helix-coil transition width were calculated from the melting curves. A phenomenological approach was used to describe the melting behavior of the fibers in and around the B-A transition region. The effect of netropsin on the melting of DNA fibers was attributed mainly to the stabilization of B-DNA and to a higher melting cooperativity in the B-DNA region.     

Mapping the B-A conformational transition along plasmid DNA

A simple method is presented to monitor conformational isomerizations along genomic DNA. We illustrate properties of the method with the B-A conformational transition induced by ethanol in linearized pUC19 plasmid DNA. At various ethanol concentrations, the DNA was irradiated with ultraviolet light, transferred to a restriction endonuclease buffer and the irradiated DNA was cleaved by 17 restriction endonucleases. The irradiation damaged DNA and the damage blocked the restrictase cleavage. The amount of uncleaved, i.e. damaged, DNA depended on the concentration of ethanol in a characteristic S-shape way typical of the cooperative B-A transition. The transition beginning and midpoint were determined for each restriction endonuclease. These data map the B-A transition along the whole polylinker of pUC19 DNA and six evenly distributed recognition sequences within the rest of the plasmid. The transition midpoints fell within the B-A transition region of the plasmid simultaneously determined by CD spectroscopy. The present method complements the previous methods used to study the B-A transition. It can be employed to analyze multikilobase regions of genomic DNA whose restriction endonuclease cleavage fragments can be separated and quantified on agarose gels.     

Properties of supercoiled DNA in gel electrophoresis. The V-like dependence of mobility on topological constraint. DNA-matrix interactions

The dependence of the electrophoretic mobility of small DNA rings on topological constraint was investigated in acrylamide or agarose gels as a function of DNA size (from approximately 350 to 1400 base-pairs), gel concentration and nucleotide sequence. Under appropriate adjustment between the size of the DNA and the gel concentration, this dependence was found to be V-shaped in a limited interval around constraint O, the minimum mobility at the apex of the V being obtained for relaxed DNA. Analysis of the DNA size dependence of the V suggests that it is the result of a modulated compaction of the DNA rings by the gel matrix. Compaction appears to be maximum upon relaxation, and to decrease with increase in supercoiling. Consistent with this interpretation, gels were found to oppose structural departures from the B helix, such as Z transition and cruciform extrusion, which tend to relax the DNA molecule and make it more expanded. In contrast, when DNA size or gel concentration are large enough relative to one another, U shapes are observed instead of Vs, as a consequence of an increase in the mobility of the rings closer to relaxation. The relevance of these results to the situation of superhelical DNA in vivo is discussed. Application of the V to the measurement of the DNA helical twist is mentioned.     

The B-A transition in superhelical DNA.

Relaxation of a DNA superhelical stress due to the B to A transition induced by trifluoroethanol has been studied by assessing the change of DNA orientation in a flow gradient. Using DNAs of different superhelical densities, a decrease in the winding angle during the B----A shift of DNA was found to be 1.5 degrees per base pair in solution. Accepting the winding angle for B-DNA in solution to be 34.1 degrees, that for A-DNA must have a value of 32.6 degrees which agrees with the X-ray data for A-DNA in the condensed state. The date obtained within the B-A transition interval make it possible to conclude that there is an increase in winding at each B/A junction, which is about 5 degrees per one junction.     

CC/GG contacts facilitate the B to A transition of DNA in solution

Self-complementary decadeoxynucleotides, CCGATATCGG, CCAGATCTGG, CCCTGCAGGG, GGGGGCCCCC, were designed and synthesized to estimate the A-philic free energy of CC/GG contacts. First, regions of temperature-stability of the double-stranded conformation were determined for each 10-mer. Then, circular dichroism spectra were recorded for the B-family forms at different temperatures, counter-ion concentrations and trifluoroethanol contents. A cooperative change typical of the B-A transition is observed in the CD spectra at a trifluoroethanol content specific for each duplex. The positions of half-transition points were functions not only of the nucleotide sequence but of the duplex length as well: the B to A transitions were hindered in these 10-mers in comparison with a lengthy DNA. The B-phility value was estimated to be 3 kcal/mol of 10-mer. The B-A transition point was shown to drop with an increase in the number of CC/GG contacts in a duplex. The designed 10-mers made it possible to estimate quantitatively the A-phility of CC/GG contact as compared with an average DNA: (FA-FB)CC = 0.2 Kcal/mol, (FA-FB)DNA = 0.7 Kcal/mol.     

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.     

Theory of Low-Frequency Vibrations in DNA Macromolecules

Abstract

To describe low-frequency dynamics of DNA macromolecules a model is developed taking into account the hydrogen bond stretching in base pairs, the backbone flexibility and intranucleoside mobility. For double-stranded DNA the normal vibrations are found and the structure of low- frequency spectrum is determined. The agreement between theory and Raman spectroscopy data for B-DNA is demonstrated. Conformational dependences of vibration spectrum during the B→A and helix→coil DNA transitions are studied. The contribution coming from low-frequency mobility to the nucleic-protein recognition processes is discussed.     

The sequence-directed bent DNA detected in the replication origin of Chlamydomonas reinhardtii chloroplast DNA is important for the replication function

Summary We demonstrated that the 1055 by restriction fragment containing OriA, a chloroplast DNA replication origin of Chlamydomonas reinhardtii, has electrophoretic anomalies characteristic of bent DNA. A tandem dimer of the region was constructed. Quantitative measurement of the relative gel mobility of a set of permuted fragments was used to extrapolate the approximate position of the bent DNA segment. By analyzing the gel mobility of short, sequenced fragments of the bent DNA region, the putative bending locus was identified. Two A₄ tracts and two A5 tracts were located in the bending locus. Oligonucleotide-directed mutagenesis was then used to disrupt the A tract or the spacing between A tracts and the effect of site-specific mutation on electrophoretic mobility was analyzed. To assess the functional role of the bent DNA region, subclones containing the bending locus, mutated bending locus, and regions flanking the bending locus were constructed. Each subclone was used as template in an in vitro DNA replication system which preferentially initiated DNA replication at OriA. A 224 by subclone with the bending locus positioned in the middle displayed the highest replication function and was sufficient to initiate DNA replication in vitro. Site-specific mutations or alterations of the A tracts resulted in decreased DNA bending and decreased DNA replication activity.