1H NMR investigation of the conformational states of DNA in nucleosome core particles.

In this study 1H NMR has been used to investigate the conformational state of DNA in nucleosome core particles. The nucleosome core particles exhibit partially resolved low field (10-15 ppm) spectra due to imino protons in Watson-Crick base pairs (one resonance per GC or AT base pair). To a first approximation, the spectrum is virtually identical with that of protein-free 140 base pair DNA, and from this observation we draw two important conclusions: (i) Since the low field spectra of DNA are known to be sensitive to conformation, the conformation of DNA in the core particles is essentially the same as that of free DNA (presumably B-form), (ii) since kinks occurring at a frequency at 1 in 10 or 1 in 20 base pairs would result in a core particle spectrum different from that of free DNA we find no NMR evidence supporting either the Crick-Klug or the Sobell models for kinking DNA around the core histones. Linewidth considerations indicate that the rotational correlation time for the core particles is approximately 1.5 X 10(-7) sec, whereas the end-over-end tumbling time of the free 140 base pair DNA is 3 X 10(-7) sec.     

DNA oligonucleotides with A, T, G or C opposite an abasic site: structure and dynamics

Abasic sites are common DNA lesions resulting from spontaneous depurination and excision of damaged nucleobases by DNA repair enzymes. However, the influence of the local sequence context on the structure of the abasic site and ultimately, its recognition and repair, remains elusive. In the present study, duplex DNAs with three different bases (G, C or T) opposite an abasic site have been synthesized in the same sequence context (5′-CCA AAG₆ XA₈C CGG G-3′, where X denotes the abasic site) and characterized by 2D NMR spectroscopy. Studies on a duplex DNA with an A opposite the abasic site in the same sequence has recently been reported [Chen,J., Dupradeau,F.-Y., Case,D.A., Turner,C.J. and Stubbe,J. (2007) Nuclear magnetic resonance structural studies and molecular modeling of duplex DNA containing normal and 4′-oxidized abasic sites. Biochemistry, 46, 3096–3107]. Molecular modeling based on NMR-derived distance and dihedral angle restraints and molecular dynamics calculations have been applied to determine structural models and conformational flexibility of each duplex. The results indicate that all four duplexes adopt an overall B-form conformation with each unpaired base stacked between adjacent bases intrahelically. The conformation around the abasic site is more perturbed when the base opposite to the lesion is a pyrimidine (C or T) than a purine (G or A). In both the former cases, the neighboring base pairs (G6-C21 and A8-T19) are closer to each other than those in B-form DNA. Molecular dynamics simulations reveal that transient H-bond interactions between the unpaired pyrimidine (C20 or T20) and the base 3′ to the abasic site play an important role in perturbing the local conformation. These results provide structural insight into the dynamics of abasic sites that are intrinsically modulated by the bases opposite the abasic site.     

How hormone receptor-DNA binding affects nucleosomal DNA: the role of symmetry.

Molecular dynamics simulations have been employed to determine the optimal conformation of an estrogen receptor DNA binding domain dimer bound to a consensus response element, ds(AGGTCACAGTGACCT), and to a nonconsensus response element, ds(AGAACACAGTGACCT). The structures simulated were derived from a crystallographic structure and solvated by a sphere (45-A radius) of explicit water and counterions. Long-range electrostatic interactions were accounted for during 100-ps simulations by means of a fast multipole expansion algorithm combined with a multiple time-step scheme in the molecular dynamics package NAMD. The simulations demonstrate that the dimer induces a bent and underwound (10.7 bp/turn) conformation in the DNA. The bending reflects the dyad symmetry of the receptor dimer and can be described as an S-shaped curve in the helical axis of DNA when projected onto a plane. A similar bent and underwound conformation is observed for nucleosomal DNA near the nucleosome's dyad axis that reflects the symmetry of the histone octamer. We propose that when a receptor dimer binds to a nucleosome, the most favorable dimer-DNA and histone-DNA interactions are achieved if the respective symmetry axes are aligned. Such positioning of a receptor dimer over the dyad of nucleosome B in the mouse mammary tumor virus promoter is in agreement with experiment.     

The absence of non-local conformational changes in OR3 operator DNA on complexing with the cro repressor

The Interaction of the cro protein of lambda phage with a synthetic OR3 operator having 17 base pairs in length and with its 9 bp fragment has been studied using the circular dichroism (CD) method. In both cases, a considerable change in the CD of the samples was found in the region 260-300 nm upon the addition of the cro protein. The stoichiometry obtained by the CD titration was identical for OR3 and its 9 bp fragment: one duplex per dimeric cro. NaCl addition makes the complexes dissociate so that the 9 bp fragment becomes free at [NaCl] greater than 0.2 M while the whole OR3 becomes free at [NaCl] greater than 0.5 M. The CD spectra of both the free duplexes show a typical B-form conservative pattern with a positive CD band (270 nm) and a negative one (250 nm). The specific complexing of both the duplexes results in a substantial CD depression in the positive band. The most pronounced effect occurs at 280 nm. This spectral change is quite distinct from those in the B to A transition and in the non-cooperative winding of the DNA within the B-family of forms. The interaction of the cro protein with the non-operator DNAs, calf thymus DNA and a synthetic 10 bp duplex, reveals no visible CD changes at all. An inference is drawn that the CD change in the specific complexes is mainly due to the induced CD in tyr-26 upon its interaction with a specific base pair in the operator or its fragment, the operator DNA conformation being conserved in a B-like form as a whole.(ABSTRACT TRUNCATED AT 250 WORDS)     

Synapsis of recombination signal sequences located in cis and DNA underwinding in V(D)J recombination

V(D)J recombination requires binding and synapsis of a complementary (12/23) pair of recombination signal sequences (RSSs) by the RAG1 and RAG2 proteins, aided by a high-mobility group protein, HMG1 or HMG2. Double-strand DNA cleavage within this synaptic, or paired, complex is thought to involve DNA distortion or melting near the site of cleavage. Although V(D)J recombination normally occurs between RSSs located on the same DNA molecule (in cis), all previous studies that directly assessed RSS synapsis were performed with the two DNA substrates in trans. To overcome this limitation, we have developed a facilitated circularization assay using DNA substrates of reduced length to assess synapsis of RSSs in cis. We show that a 12/23 pair of RSSs is the preferred substrate for synapsis of cis RSSs and that the efficiency of pairing is dependent upon RAG1-RAG2 stoichiometry. Synapsis in cis occurs rapidly and is kinetically favored over synapsis of RSSs located in trans. This experimental system also allowed the generation of underwound DNA substrates containing pairs of RSSs in cis. Importantly, we found that the RAG proteins cleave such substrates substantially more efficiently than relaxed substrates and that underwinding may enhance RSS synapsis as well as RAG1/2-mediated catalysis. The energy stored in such underwound substrates may be used in the generation of DNA distortion and/or protein conformational changes needed for synapsis and cleavage. We propose that this unwinding is uniquely sensed during synapsis of an appropriate 12/23 pair of RSSs.     

The structure of recA protein-DNA filaments. 2 recA protein monomers unwind 17 base pairs of DNA by 11.5 degrees/base pair in the presence of adenosine 5'-O-(3-thiotriphosphate)

recA protein binds to duplex DNA in the presence of Mg2+ and adenosine 5'-O-(3-thiotriphosphate) forming a stiff nucleoprotein filament with a distinct axial repeat which contains 17 +/- 1 base pairs and spans 8-9 nm along the fiber (Di Capua, E., Engel, A., Stasiak, A., and Koller, Th. (1982) J. Mol. Biol. 157, 87-103; Dunn, K., Chrysogelos, S., and Griffith, J. (1982) Cell 28, 757-765). Measurement of the protein:DNA ratio in these filaments utilizing double label analysis and isopycnic density banding shows that there are 2 recA monomers for every 17 base pairs. The DNA is also partially unwound in this filament. Utilizing the recA-induced relaxation of naturally supertwisted SV40 DNA, we show that the DNA is unwound by 11.5 +/- 1.5 degrees/base pair which corresponds to 180-200 degrees for each repeat unit along the filament length.     

1H NMR study of the interaction of bacteriophage lambda Cro protein with the OR3 operator. Evidence for a change of the conformation of the OR3 operator on binding.

The specific complex between the lambda phage OR3 operator and the Cro protein has been studied by proton NMR spectroscopy at 500 MHz. The DNA imino proton resonances of this complex have been assigned to specific base pairs using the known assignments of these resonances for the free operator. Increase of the protein/DNA ratio to complete saturation of the OR3 operator with the Cro protein made it possible to follow the shift changes of the resonances. Ambiguities were resolved by nuclear Overhauser effect measurements on the complex. The shifts of the imino proton resonance positions provide information on the changes induced in the conformation of the operator upon complex formation with a dimer of the Cro protein. The most striking shift occurs for the central (GC 9) base pair, which is known to have no direct contacts with the Cro protein. This shift may be induced by a bend in the OR3 operator DNA at the GC 9 base pair to accommodate the operator for the binding of the Cro protein dimer. The imino proton resonances of two additional base pairs can be observed in the complex, demonstrating an overall stabilization of the DNA structure by the binding of the Cro protein.     

Solution structure of the dodecamer d-(CATGGGCC-CATG)2 is B-DNA. Experimental and molecular dynamics study

The DNA duplex d-(CATGGGCCCATG)2 has been studied in solution by FTIR, NMR and CD. The experimental approaches have been complemented by series of large-scale unrestrained molecular dynamics simulation with explicit inclusion of solvent and counterions. Typical proton-proton distances extracted from the NMR spectra and the CD spectra are completely in agreement with slightly modified B-DNA. By molecular dynamics simulation, starting from A-type sugar pucker, a spontaneous repuckering to B-type sugar pucker was observed. Both experimental and theoretical approaches suggest for the dodecamer d-(CATGGGCCCATG)2 under solution conditions puckering of all 2'-deoxyribose residues in the south conformation (mostly C2'-endo) and can exclude significant population of sugars in the north conformation (C3'-endo). NMR, FTIR and CD data are in agreement with a B-form of the dodecamer in solution. Furthermore, the duplex shows a cooperative B-A transition in solution induced by addition of trifluorethanol. This contrasts a recently published crystal structure of the same oligonucleotide found as an intermediate between B- and A-DNA where 23 out of 24 sugar residues were reported to adopt the north (N-type) conformation (C3'-endo) like in A-DNA (Ng, H. L., Kopka, M. L. and Dickerson, R. E., Proc. Natl. Acad. Sci. U S A 97, 2035-2039 (2000)). The simulated structures resemble standard B-DNA. They nevertheless show a moderate shift towards A-type stacking similar to that seen in the crystal, despite the striking difference in sugar puckers between the MD and X-ray structures. This is in agreement with preceding MD reports noticing special stacking features of G-tracts exhibiting a tendency towards the A-type stacking supported by the CD spectra also reflecting the G-tract stacking. MD simulations reveal several noticeable local conformational variations, such as redistribution of helical twist and base pair roll between the central GpC steps and the adjacent G-tract segments, as well as a substantial helical twist variability in the CpA(TpG) steps combined with a large positive base pair roll. These local variations are rather different from those seen in the crystal.