Determination of the extent of DNA bending by an adenine-thymine tract

We determined the magnitude of the bend induced in DNA by an adenine-thymine tract by measuring the rate of cyclization of DNA oligonucleotides containing phased A tracts. A series of linear multimers with 2-bp single-stranded ends, in which the (A.T)6 tracts are separated by CG2-3C sequences and are positioned 10 and 11 bp apart alternately, were prepared from 21 bp long synthetic duplexed deoxyoligonucleotides. The cyclization rates of the multimers (105-210 bp) and the bimolecular association rate of the 84 bp long multimer were measured in the presence of DNA ligase. From the rate constants of the cyclization and bimolecular association reactions, ring closure probabilities were obtained for the multimers. The systematically bent molecules were simulated by Monte Carlo methods, and the ring closure probabilities were calculated for a given set of junction bend angles. By comparing the calculated values of ring closure probabilities to experimental values and adjusting the junction bend angles to fit experimental values, the extent of bending at the junctions (or the extent of bending for an adenine tract) was determined. We conclude that an A6 tract bends the DNA helix by 17-21 degrees.     

Structural basis of stable bending in DNA containing An tracts. Different types of bending

Structural determinants of DNA bending of different types have been studied by theoretical conformational analysis of duplexes. Their terminal parts were fixed either in an ordinary low-energy B-like conformation or in "anomalous" conformations with a narrowed minor groove typical of An tracts. The anomalous conformations had different negative tilt angles (up to about zero), different propeller twists and minor groove widths. Calculations have been performed for DNA fragments AnTm, TnAm, AnGCTm, AnCGTm, TmGCAn, TmCGAn which are the models of the junction of two anomalous structures on An and Tm tracts. On the AT step of the AnTm fragment the minor groove can be easily narrowed so that a whole unbent fragment of anomalous structure is formed on AnTm. According to our energy estimates, there should not be any reliable bending on AnTm. In contrast, in all other cases there was a pronounced roll-like bending into the major groove in the chemical symmetry region. Calculations of the junction between the anomalous and ordinary B-like structure for GnTm and CnAm have shown that there is an equilibrium bending with a tilt component towards the chain having the anomalous structure at the 5'-end. From our calculations it is impossible to determine precisely the direction of bending, though it can be suggested that the roll component of bending might be directed towards the major groove. The anomalous structure is the main reason of bending; alternations of pyrimidines and purines can modulate the value and the direction of equilibrium bending (only the value in the case of self-complementary fragments).(ABSTRACT TRUNCATED AT 250 WORDS)     

The adenine-thymine domain of the simian virus 40 core origin directs DNA bending and coordinately regulates DNA replication.

The simian virus 40 origin of replication contains a 20-base-pair adenine-thymine-rich segment with the sequence 5'-TGCATAAATAAAAAAAATTA-3'. The continuous tract of eight adenines is highly conserved among polyomaviruses. We used single-base substitutions to map structural and functional features of this DNA. Mutations in the AAA and AAAAAAAATT sequences significantly reduce DNA replication and thus identify two sequence-specific functional domains or a single domain with two parts. The AAAAAAAATT sequence also determines a DNA conformation that is characteristic of DNA bending. Single-base mutations in this domain change the degree of net bending, presumably by altering the length and location of the bending sequence. Thus, DNA bending in the correct conformation and location may be a structural signal for replication in polyomavirus origins and perhaps in other origins of replication with consecutive runs of adenines. The first five base pairs (TGCAT) of the 20-base-pair segment and the T between the AAA and AAAAAAAATT domains serve a sequence-independent function that may establish proper spacing within the core origin.     

DNA binding and bending by HMG boxes: energetic determinants of specificity

To clarify the physical basis of DNA binding specificity, the thermodynamic properties and DNA binding and bending abilities of the DNA binding domains (DBDs) of sequence-specific (SS) and non-sequence-specific (NSS) HMG box proteins were studied with various DNA recognition sequences using micro-calorimetric and optical methods. Temperature-induced unfolding of the free DBDs showed that their structure does not represent a single cooperative unit but is subdivided into two (in the case of NSS DBDs) or three (in the case of SS DBDs) sub-domains, which differ in stability. Both types of HMG box, most particularly SS, are partially unfolded even at room temperature but association with DNA results in stabilization and cooperation of all the sub-domains. Binding and bending measurements using fluorescence spectroscopy over a range of ionic strengths, combined with calorimetric data, allowed separation of the electrostatic and non-electrostatic components of the Gibbs energies of DNA binding, yielding their enthalpic and entropic terms and an estimate of their contributions to DNA binding and bending. In all cases electrostatic interactions dominate non-electrostatic in the association of a DBD with DNA. The main difference between SS and NSS complexes is that SS are formed with an enthalpy close to zero and a negative heat capacity effect, while NSS are formed with a very positive enthalpy and a positive heat capacity effect. This indicates that formation of SS HMG box-DNA complexes is specified by extensive van der Waals contacts between apolar groups, i.e. a more tightly packed interface forms than in NSS complexes. The other principal difference is that DNA bending by the NSS DBDs is driven almost entirely by the electrostatic component of the binding energy, while DNA bending by SS DBDs is driven mainly by the non-electrostatic component. The basic extensions of both categories of HMG box play a similar role in DNA binding and bending, making solely electrostatic interactions with the DNA.     

DNA curvature at A tracts containing a non-polar thymine mimic

We report the first experimental probing of electrostatic interactions on the pyrimidine side of a bent A tract. Although the curvature of short A tracts (A₄–A₆) has long been studied, its physical origins remain under debate. Current hypotheses include the influence of major-groove hydrogen bonds between propeller-twisted base pairs, electrostatic effects of closely associated minor-groove cations, effects of minor-groove solvation, and stacking effects at the junctions adjacent to the A tract. We investigated this problem through the substitution of thymidines in A₅ tracts by difluorotoluene deoxynucleoside (F), a non-polar molecule of the same size and shape which lacks hydrogen bonding and metal-ion complexing capabilities. Ligation experiments with phased A tracts demonstrated that F substitution has asymmetric effects on the bend angle. The strongest effects occurred at the second and third thymines where curvature was reduced from 19.8° to 5.3° and 9.6°, respectively. Moderate effects were observed with substitutions at positions 1 and 4, while substitution at position 5 had no effect on bend angle. The results support the hypothesis that highly localized electrostatic interactions are a principal cause of A-tract curvature. Furthermore, they are most consistent with the notion that local metal-ion complexation at O2 of thymine is a strong component of these interactions.     

Physical studies of DNA premelting equilibria in duplexes with and without homo dA.dT tracts: correlations with DNA bending

We have employed a variety of physical methods to study the equilibrium melting and temperature-dependent conformational dynamics of dA.dT tracts in fractionated synthetic DNA polymers and in well-defined fragments of kinetoplast DNA (kDNA). Using circular dichroism (CD), we have detected a temperature-dependent, "premelting" event in poly(dA).poly(dT) which exhibits a midpoint near 37 degrees C. Significantly, we also detect this CD "premelting" behavior in a fragment of kDNA. By contrast, we do not observe this "premelting" behavior in the temperature-dependent CD spectra of poly[d(AT)].poly[d(AT)], poly(dG).poly(dC), poly[d(GC)].poly[d(GC)], or calf thymus DNA. Thus, poly(dA).poly(dT) and kDNA exhibit a common CD-detected "premelting" event which is absent in the other duplex systems studied in this work. Furthermore, we find that the anomalous electrophoretic retardation of the kDNA fragments we have investigated disappears at temperatures above approximately 37 degrees C. We also observe that the rotational dynamics of poly(dA).poly(dT) and kDNA as assessed by singlet depletion anisotropy decay (SDAD) and electric birefringence decay (EBD) also display a discontinuity near 37 degrees C, which is not observed for the other duplex systems studied. Thus, in the aggregate, our static and dynamic measurements suggest that the homo dA.dT sequence element [common to both poly(dA).poly(dT) and kDNA] is capable of a temperature-dependent equilibrium between at least two helical states in a temperature range well below that required to induce global melting of the host duplex. We suggest that this "preglobal" melting event may correspond to the thermally induced "disruption" of "bent" DNA.     

Structural alteration in alternating adenine-thymine sequences in positively supercoiled DNA

An alternating adenine-thymine tract in a relaxed closed circular plasmid was found to become strongly reactive to osmium tetroxide in the presence of actinomycin D. We suggest that this is due to a local overwinding of the alternating tract as a result of positive supercoiling induced by intercalation of the antibiotic at GpC sequences elsewhere in the DNA. We have previously shown that (A.T)n sequences undergo a local underwinding in response to negative supercoiling, and it appears that such sequences are especially torsionally deformable in both directions.     

Supercoiling-induced DNA bending

Local DNA bending is a critical factor for numerous DNA functions including recognition of DNA by sequence-specific regulatory binding proteins. Negative DNA supercoiling increases both local and global DNA dynamics, and this dynamic flexibility can facilitate the formation of DNA-protein complexes. We have recently shown that apexes of supercoiled DNA molecules are sites that can promote the formation of an alternative DNA structure, a cruciform, suggesting that these positions in supercoiled DNA are under additional stress and perhaps have a distorted DNA geometry. To test this hypothesis, we used atomic force microscopy to directly measure the curvature of apical positions in supercoiled DNA. The measurements were performed for an inherently curved sequence formed by phased A tracts and a region of mixed sequence DNA. For this, we used plasmids in which an inverted repeat and A tract were placed at precise locations relative to each other. Under specific conditions, the inverted repeat formed a cruciform that was used as a marker for the unambiguous identification of the A tract location. When the A tract and cruciform were placed diametrically opposite, this yielded predominantly nonbranched plectonemic molecules with an extruded cruciform and A tract localized in the terminal loops. For both the curved A tract and mixed sequence nonbent DNA, their localization to an apex increased the angle of bending compared to that expected for DNA unconstrained in solution. This is consistent with increased helical distortion at an apical bend.     

The Raman spectra of left-handed DNA oligomers incorporating adenine-thymine base pairs+.

Raman spectra were obtained from single crystals of [d(CGCATGCG)]2 and [d(m5CGTAm5CG)]2, both of which incorporate A-T pairs into Z-DNA structures and contain C2'-endo/syn conformers of deoxyguanosine at the oligonucleotide ends. Correlation with x-ray results permits the following Raman assignments for nucleoside conformers: C3'-endo/syn G, 623 +/- 1; C2'-endo/syn G, 671 +/- 2; C2'-endo/anti C, 782 +/- 1; C2'endo/anti T, 650 +/- 5 and ca. 750; C3'-endo/syn A, 729 +/- 1 cm-1. These results show that (i) the 670 cm-1 line of syn G is highly sensitive to the change from C3'-endo to C2'-endo pucker, (ii) the 729 cm-1 line of A is affected neither by furanose pucker nor glycosidic bond orientation and (iii) the 1200-1500 cm-1 region of the Raman spectrum of the A-T double helix is greatly altered by the B-to-Z transition. Conformation sensitive Raman frequencies in the 850-1700 cm-1 region are identified for both octamer and hexamer, and the Z-to-B transition of each is monitored by spectral changes which occur upon dissolving the crystal in H2O solution.     

Mechanisms of DNA bending

Genome packaging and gene regulation require DNA bending. Recent developments in the elucidation of the mechanisms involved in DNA bending include new X-ray structures (most notably that of the mammalian nucleosome) wherein DNA is bent, controversy surrounding interpretation of DNA-bending experiments with basic-leucine zipper proteins, studies of electrostatic effects in DNA bending, and the design of artificial DNA-bending ligands.     

Phased adenine tracts in double-stranded RNA do not induce sequence-directed bending

Tracts of four to six adenines phased with the DNA helix produce a sequence-directed bending of the helix axis. Here, using gel electrophoresis and electron microscopy (EM), we have asked whether a similar motif will induce bending in a duplex RNA helix. Single-stranded RNAs were transcribed either from short synthetic DNA templates or from Crithidia fasciculata kinetoplast bent DNA, and the complementary single-stranded RNAs were annealed to produce duplex RNA molecules containing blocks of four to six adenines. Electrophoresis on polyacrylamide gels revealed no retardation of the RNAs containing phased blocks of adenines relative to duplex RNAs lacking such blocks. Examination by EM showed most of the molecules to be straight or only slightly bent. Thus, in contrast to DNA duplexes, phased adenine tracts do not induce sequence-directed bending in double-stranded RNA. Analysis of the distribution of molecule shapes for the highly bent C. fasciculata DNA showed that the adenine blocks do not act cooperatively to induce DNA bending and that the molecules must equilibrate between a spectrum of bent shapes.     

Dynamic bending rigidity of DNA

Rapidly relaxing components in the decay of the transient electric dichroism of DNA restriction fragments were reported by Diekmann et al. [(1982) Biophys. Chem. 15, 263-270] and P?rschke et al. [(1987) Biopolymers 26, 1971-1974]. These are analyzed using a new normal mode theory for weakly bending rods and assigned to bending. The longest bending relaxation times for fragments with 95-250 base pairs coincide with the theoretical curve calculated for a dynamic bending rigidity corresponding to a dynamic persistence length Pd = 2100 A. Analysis of the relative amplitudes of fast and slow components following weak orienting pulses is also consistent with a rather large dynamic persistence length. The enhancement of the relative amplitude of the fast component in large electric fields is attributed to steady-state bending of initially perpendicular DNAs by the field. Several reasons are proposed why the dynamic bending rigidity is 4 times larger than the apparent static bending rigidity inferred from equilibrium persistence length measurements on the same fragments.     

Intrinsic bending in GGCC tracts as probed by fluorescence resonance energy transfer

Double-stranded oligonucleotides containing the sequence 5'-GGCC-3' can be intrinsically bent, according to X-ray crystallography and gel electrophoresis mobility studies. We have performed fluorescence resonance energy transfer (FRET) experiments with dye-labeled oligonucleotides to further investigate the solution structure of this sequence. We find that 5'-GGCC-3'-containing oligonucleotides bring 5'-attached donor and acceptor dyes much closer together than a comparable "straight" sequence that contains 5'-GCGC-3'. The bend angle for the 5'-GGCC-3' sequence is estimated to be approximately 70 degrees, much larger than the crystallographically observed 23 degrees kink but in agreement with other FRET work. In contrast to gel electrophoresis studies, divalent metal ions do not promote increased kinking in 5'-GGCC-3' above background as judged by FRET. Thus, sequence-dependent structural effects in DNA may be a complicating feature of FRET experiments.