Conformational changes in the oligonucleotide duplex d(GCGTTGCG) x d(CGCAACGC) induced by formation of a cis-syn thymine dimer. A two-dimensional NMR study

In order to obtain insight into the repair mechanism of DNA containing thymine photo-dimer, the conformation of the duplex d(GCGTTGCG) x d(CGCAACGC) with a thymine dimer incorporated has been studied by proton NMR and the results are compared with NMR data of the parent octamer. Two-dimensional nuclear Overhauser enhancement (2D NOE) spectroscopy and two-dimensional homonuclear Hartmann-Hahn spectroscopy have been applied to assign all the non-exchangeable base protons and most of the deoxyribose protons of both duplexes. From these experiments it is clear that indeed a cis-syn cyclobutane-type thymine photodimer is formed by the irradiation of this oligonucleotide with ultraviolet light. Comparison of 2D NOE spectra and the 1H chemical shifts of the damaged and the intact DNA duplexes reveals that formation of a thymine dimer induces small distortions of the B-DNA structure, the main conformational change occurring at the site of the thymine dimer.     

The effect of two antipodal fluorine-induced sugar puckers on the conformation and stability of the Dickerson-Drew dodecamer duplex [d(CGCGAATTCGCG)]2.

UV thermal melting studies, CD and NMR spectroscopies were employed to assess the contribution of antipodal sugar conformations on the stability of the canonical B-DNA conformation of the Dickerson-Drew dodecamer duplex [[d(CGCGAATTCGCG)]2, (ODN 1)]. Different oligodeoxynucleotide versions of ODN 1 were synthesized with modified thymidine units favoring distinct sugar conformations by using a 3'- endo (north) 2'-fluoro-2'-deoxyribofuranosyl thymine (1) or a 2'- endo (south) 2'-fluoro-2'-deoxyarabinofuranosyl thymine (2). The results showed that two south thymidines greatly stabilized the double helix, whereas two north thymidines destabilized it by inducing a more A-like conformation in the middle of the duplex. Use of combinations of north and south thymidine conformers in the same oligo destabilized the double helix even further, but without inducing a conformational change. The critical length for establishing a detectable A-like conformation in the middle of a B-DNA ODN appears to be 4 bp. Our results suggest that manipulation of the conformation of DNA in a sequence-independent manner is possible.     

1H NMR study of the exchangeable protons of the duplex d(GCGTTGCG).d(CGCAACGC) containing a thymine photodimer.

A comparison is presented of the imino proton NMR spectra of the double stranded octamer d(GCGTTGCG).d(CGCAACGC) and the same octamer in which the two central thymine residues occur as a cis-syn thymine dimer. Except for the terminal base pairs all imino protons were detected and assigned in the NMR spectrum. The spectra show that in the thymine dimer duplex, contrary to common belief, all base pairs occur in a hydrogen bonded form, although the hydrogen bonds of the two central AT base pairs are substantially weakened. The melting temperature decreases about 13 degrees C on thymine dimer formation.     

RNA-like conformational properties of a synthetic DNA poly(dA-dU).poly(dA-dU)

Differences in the circular dichroism of poly(dA-dT).poly(dA-dT) and poly(dA-dU).poly(dA-dU) and in its temperature induced changes are reported. A comparison to the data obtained with DNA and RNA indicates that an absence of thymine methyl groups in the polynucleotide results in promoting its RNA-like conformational properties. However, poly(dA-dU).poly(dA-dU) is not an A-DNA type of double helix.     

Two-dimensional proton nuclear magnetic resonance investigation of the synthetic deoxyribonucleic acid decamer d(ATATCGATAT)2

In this study two-dimensional NMR techniques (COSY and NOESY) have been used in conjunction with one-dimensional NMR results to complete the assignment of the proton NMR spectrum of the double-stranded DNA decamer, d(ATATCGATAT)2, and to obtain qualitative information about numerous interproton distances in this molecule and some limited information about conformational dynamics. COSY and NOESY measurements have been combined to systematically assign many of the resonances from the H1' and H2',2" sugar protons to specific nucleotides in the double helix. This method relies on the fact that sugar protons within a specific nucleotide are scalar coupled and that base protons (AH8, GH8, TH6, and CH6) in right-handed helices can interact simultaneously with their own H2',2" sugar protons and those of the adjacent (5'-3') nucleotide attached to its 5' side (i.e., XpA not ApX). A COSY experiment is used to identify sugar resonances within a residue whereas the NOESY experiment allows the neighboring sugar to be connected (linked). The CH5 and CH6 resonances in the spectrum can immediately be identified by the COSY experiment. The methyl protons of thymine residues exhibit strong through-space interbase interactions both with their own TH6 proton and with AH8 proton on the adjacent (5'-3') adenine residue. These interactions are used both to make assignments of the spectra and to establish that the thymine methyl groups are in close proximity to the AH8 protons of adjacent adenine residues [Feigon, J., Wright, J. M., Leupin, W., Denny, W. A., & Kearns, D. R. (1982) J. Am. Chem. Soc. 104, 5540].(ABSTRACT TRUNCATED AT 250 WORDS)     

Sequence-dependent conformation of an A-DNA double helix. The crystal structure of the octamer d(G-G-T-A-T-A-C-C)

The crystal structures of the synthetic self-complementary octamer d(G-G-T-A-T-A-C-C) and its 5-bromouracil-containing analogue have been refined to R values of 20% and 14% at resolutions of 1.8 and 2.25 A, respectively. The molecules adopt and A-DNA type double-helical conformation, which is minimally affected by crystal forces. A detailed analysis of the structure shows a considerable influence of the nucleotide sequence on the base-pair stacking patterns. In particular, the electrostatic stacking interactions between adjacent guanine and thymine bases produce symmetric bending of the double helix and a major-groove widening. The sugar-phosphate backbone appears to be only slightly affected by the base sequence. The local variations in the base-pair orientation are brought about by correlated adjustments in the backbone torsion angles and the glycosidic orientation. Sequence-dependent conformational variations of the type observed here may contribute to the specificity of certain protein-DNA interactions.     

Structure of d(T)n.d(A)n.d(T)n: the DNA triple helix has B-form geometry with C2'-endo sugar pucker.

The polynucleotide helix d(T)n.d(A)n.d(T)n is the only deoxypolynucleotide triple helix for which a structure has been published, and it is generally assumed as the structural basis for studies of DNA triplexes. The helix has been assigned to an A-form conformation with C3'-endo sugar pucker by Arnott and Selsing [1974; cf. Arnott et al. (1976)]. We show here by infrared spectroscopy in D2O solution that the helix is instead B-form and that the sugar pucker is in the C2'-endo region. Distamycin A, which binds only to B-form and not to A-form helices, binds to the triple helix without displacement of the third strand, as demonstrated by CD spectroscopy and gel electrophoresis. Molecular modeling shows that a stereochemically satisfactory structure can be build using C2'-endo sugars and a displacement of the Watson-Crick base-pair center from the helix axis of 2.5 A. Helical constraints of rise per residue (h = 3.26 A) and residues per turn (n = 12) were taken from fiber diffraction experiments of Arnott and Selsing (1974). The conformational torsion angles are in the standard B-form range, and there are no short contacts. In contrast, we were unable to construct a stereochemically allowed model with A-form geometry and C3'-endo sugars. Arnott et al. (1976) observed that their model had short contacts (e.g., 2.3 A between the phosphate-dependent oxygen on the A strand and O2 in the Hoogsteen-paired thymine strand) which are generally known to be outside the allowed range.(ABSTRACT TRUNCATED AT 250 WORDS)     

1H NMR assignment and melting temperature study of cis-syn and trans-syn thymine dimer containing duplexes of d(CGTATTATGC).d(GCATAATACG)

The preparation and spectroscopic characterization of duplex decamers containing site-specific cis-syn and trans-syn thymine dimers are described. Three duplex decamers, d(CGTATTATGC).d(GCATAATACG), d(CGTAT[c,s]TATGC).d(GCATAATACG), and d(CGTAT[t,s]TATGC).d(GCATAATACG), were prepared by solid-phase phosphoramidite synthesis utilizing cis-syn and trans-syn cyclobutane thymine dimer building blocks (Taylor et al., 1987; Taylor & Brockie, 1988). NMR spectra (500 MHz 2D 1H and 202 MHz 1D 31P) were obtained in "100%" D2O at 10 degrees C, and 1D exchangeable 1H spectra were obtained in 10% D2O at 10 degrees C. 1H NMR assignments for H5, H6, H8, CH3, H1', H2', and H2" were made on the basis of standard sequential NOE assignment strategies and verified in part by DQF COSY data. Comparison of the chemical shift data suggests that the helix structure is perturbed more to the 3'-side of the cis-syn dimer and more to the 5'-side of the trans-syn dimer. Thermodynamic parameters for the helix in equilibrium coil equilibrium were obtained by two-state, all or none, analysis of the melting behavior of the duplexes. Analysis of the temperature dependence of the T5CH3 1H NMR signal gave delta H = 44 +/- 4 kcal and delta S = 132 +/- 13 eu for the trans-syn duplex. Analysis of the concentration and temperature dependence of UV spectra gave delta H = 64 +/- 6 kcal and delta S = 178 +/- 18 eu for the parent duplex and delta H = 66 +/- 7 kcal and delta S = 189 +/- 19 eu for cis-syn duplex. It was concluded that photodimerization of the dTpdT unit to give the cis-syn product causes little perturbation of the DNA whereas dimerization to give the trans-syn product causes much greater perturbation, possibly in the form of a kink or dislocation at the 5'-side of the dimer.     

Molecular-Mechanical studies of the mismatched base analogs of d(CGCGAATTCGCG)2:d(CGTGAATTCGCG)2, d(CGAGAATTCGCG)2, d(CGCGAATTCACG)2, d(CGCGAATTCTCG)2, and d(CGCAGAATTCGCG)·d(CGCGAATTCGCG)

Molecular-mechanical simulations have been carried out on “mismatched base” analogs of the DNA double-helical structure d(CGCGAATTCGCG)₂, in which the base pairs CG at the 3 and 10 positions have been replaced by CA, AG, TC, and TG base pairs, as well as an insertion analog in which an extra adenine has been incorporated into one strand of the above structure between bases 3 and 4. The results of these simulations (calculated relative stabilities, structures, and nmr ring-current shifts) have been compared with calorimetric and nmr data. The calculated relative stabilities of the double-helical parent dodecamer and the various “wobble” base pairs qualitatively correlate with the experimental melting temperatures. The base-pairing structure for the GT wobble pair is in agreement with that previously determined from nmr experiments. For the GA base pair, the structure with both bases anti has a slightly more favorable energy from base pairing and stacking than a structure with non-Watson-Crick H-bonding with adenine syn, in agreement with nmr experiments. The CA wobble base is calculated to favor an adenine 6NH₂ …? cytosine N3 H-bond over cytosine 4NH₂ …? adenine N1, again, in agreement with nmr experiments. There is no definitive experimental data on the TC base pair, but the existence of (somewhat long and weak) H-bonds involving cytosine 4NH₂ …? thymine 4CO and cytosine N3 …? thymine HN3 seems reasonable. We find a structure in which the extra adenine base of the insertion analogs sits “inside” the double helix.     

Conformational flexibility of B-DNA at 0.74 A resolution: d(CCAGTACTGG)(2)

The affinity and specificity of a ligand for its DNA site is a function of the conformational changes between the isolated and complexed states. Although the structures of a hydroxypyrrole-imidazole-pyrrole polyamide dimer with 5'-CCAGTACTGG-3' and the trp repressor recognizing the sequence 5'-GTACT-3' are known, the baseline conformation of the DNA site would contribute to our understanding of DNA recognition by these ligands. The 0.74 A resolution structure of a B-DNA double helix, 5'-CCAGTACTGG-3', has been determined by X-ray crystallography. Six of the nine phosphates, two of four bound calcium ions and networks of water molecules hydrating the oligonucleotide have alternate conformations. By contrast, nine of the ten bases have a single, unique conformation with hydrogen atoms visible in most cases. The polyamide molecules alter the geometry of the phosphodiester backbone, and the water molecules mediating contacts in the trp repressor/operator complex are conserved in the unliganded DNA. Furthermore, the multiple conformational states, ions and hydration revealed by this ultrahigh resolution structure of a B-form oligonucleotide are potentially general considerations for understanding DNA-binding affinity and specificity by ligands.     

Molecular dynamics simulation of the DNA triplex d(TC)5.d(GA)5.d(C+T)5.

A molecular dynamics simulation of the DNA triple helix d(TC)5.d(GA)5.d(C+T)5 is described (C+ represents a protonated cytosine residue). The simulation has been performed using the program AMBER 3.1 and includes counterions and explicit solvent under periodic boundary conditions. Both the dynamic and time-averaged behaviour of the system has been analysed. Considerable deviations from the fibre-diffraction model for DNA triple helix structure are observed, including the repuckering of the purine strand sugars that has been identified in some nuclear magnetic resonance (n.m.r.) studies. The simulation suggests that this conformational change may be driven by the possibility of improved interactions between the phosphate groups of this strand and both the solvent and counterions. Several examples of a particular conformational transition are observed, involving correlated changes in the backbone angles alpha and gamma. These transitions provide a possible explanation for some unusual n.m.r. data that have been reported. The structure of the triple helix major groove also suggests an explanation for the observed stabilization of DNA triplexes by polyvalent cations, and their ability to interact with drugs that bind in the minor groove of DNA duplexes.     

Base tilt of poly[d(A)]-poly[d(T)] and poly[d(AT)]-poly[d(AT)] in solution determined by linear dichroism

We have measured the CD, isotropic absorption, and LD of poly[d(A)]–poly[d(T)] and poly[d(AT)]–poly[d(AT)] in the vacuum-uv spectral region. The reduced dichroism (LD divided by isotropic absorption) varied as a function of wavelength and was independent of shear gradient. Thus, the bases are not perpendicular to the helix axis in solution. Since the directions of the transition dipoles are known, the orientations of the bases in the polymers can be calculated from the reduced dichroism spectra. The results show that the base normals are tilted at angles greater than 25°, with respect to the helix axis, and thymine is tilted more than adenine for both polymers. The tilt axes of adenine and thymine are not parallel, indicating a large propeller twist. Space-filling models of poly[d(A)]–poly[d(T)] and poly[(AT)]–poly[d(AT)] are built based on our results, and the conformations of the two (A + T) polymers in solution are discussed.     

Conformational polymorphism and extensibility of DNA quadruplexes formed from d(GT)n repeats

We showed earlier that oligonucleotides 3'-d(GT)5-pO(CH2CH2O)3p-d(GT)5-3' form bimolecular quadruplexes with parallel orientation of their strands, which are held by guanine quartets alternating with unpaired thymines (GT quadruplex). This work deals with the conformational polymorphism and extensibility of G quadruplexes in complex with molecules of an intercalating agent ethidium bromide (EtBr). A cooperative mechanism of EtBr binding to the GT quadruplex was revealed. The binding constant K = (3.3 +/- 0.1) x 10(4) M-1, cooperativity coefficient omega = 2.5 +/- 0.2, and maximal amount of EtBr molecules intercalated in GT quadruplex (N = 8) were determined. It was proved experimentally by analysis of adsorption isotherms and theoretically by mathematical modeling that the GT quadruplex is capable of double extension, which is indicative of the high elasticity of this four-stranded helix. Two most stable conformations of GT quadruplexes with thymine residues intercalated and/or turned outside were found by mechanico-mathematical modeling. The equilibrium is shifted toward the conformation with the looped out thymine residues upon intercalation of EtBr molecules into the GT quadruplex.     

Molecular dynamics simulation of the C-terminal sterile alpha-motif domain of human p73alpha: evidence of a dynamical relationship between helices 3 and 5

We used molecular dynamics simulation to evaluate the association properties of C-terminal sterile alpha-motif (SAM) domain of human p73alpha. To test the dimerization propensity of this structure we carried out four simulations: EphB2 X-ray dimer, p73 modeled dimer, p73 NMR monomer, and p73 modeled monomer with an elongated helix 5. The results show a direct interaction between helix 5 and helix 3 since a conformational collapse of helix 3 is observed when dimer contact and/or an elongation of helix 5 is introduced by modeling in p73 SAM domain. On the basis of these results we suggest that the recognition properties of the SAM domains may be modulated by the conformational state of helix 5.     

Characterization of a membrane protein folding motif, the Ser zipper, using designed peptides

Polar residues play important roles in the association of transmembrane helices and the stabilities of membrane proteins. Although a single Ser residue in a transmembrane helix is unable to mediate a strong association of the helices, the cooperative interactions of two or more appropriately placed serine hydroxyl groups per helix has been hypothesized to allow formation of a "serine zipper" that can stabilize transmembrane helix association. In particular, a heptad repeat Sera Xxx Xxx Leud Xxx Xxx Xxx (Xxx is a hydrophobic amino acid) appears in both antiparallel helical pairs of polytopic membrane proteins as well as the parallel helical dimerization motif found in the murine erythropoietin receptor. To examine the intrinsic conformational preferences of this motif independent of its context within a larger protein, we synthesized a peptide containing three copies of a SeraLeud heptad motif. Computational results are consistent with the designed peptide adopting either a parallel or antiparallel structure, and conformational search calculations yield the parallel dimer as the lowest energy configuration, which is also significantly more stable than the parallel trimer. Analytical ultracentrifugation indicated that the peptide exists in a monomer-dimer equilibrium in dodecylphosphocholine micelles. Thiol disulfide interchange studies showed a preference for forming parallel dimers in micelles. In phospholipid vesicles, only the parallel dimer was formed. The stability of the SerZip peptide was studied in vesicles prepared from phosphatidylcholine (PC) lipids of different chain length: POPC (C16:0C18:1 PC) and DLPC (C12:0PC). The stability was greater in POPC, which has a good match between the length of the hydrophobic region of the peptide and the bilayer length. Finally, mutation to Ala of the Ser residues in the SerZip motif gave rise to a relatively small decrease in the stability of the dimer, indicating that packing interactions rather than hydrogen-bonding provided the primary driving force for association.     

DNA flexibility as a function of allomorphic conformation and of base sequence.

Systematic theoretical modeling of symmetric DNA oligomers, carried out earlier for the B conformation, is now extended to A-DNA. In contrast to the previous results, it is found that A-DNA shows no multiplicity of low-energy substate conformations. The possibilities of the Jumna algorithm are subsequently applied to studying deformations of the oligomers. Controlled winding and stretching deformations are used to study how the two allomorphs and different base sequences absorb such external stress. The results help explain the internal mechanics of the DNA double helix and the extent to which fine structure influences this behavior. The results point to some differences between the A and B double helices, but also to many similarities. Sequence effects on flexibility are relatively limited compared to their impact on optimal energy conformations. It is also shown that the conformational substates detected for B-DNA oligomers are preserved under deformation, but have little influence on its energetics.     

Modelling extreme stretching of DNA.

Molecular modelling with Jumna is used to study extreme stretching of the DNA double helix. The results, which correlate well with recent nanomanipulation experiments, show how the double helix can be extended to twice its normal length before its base pairs break. Depending on the way the duplex is stretched two types of conformation can occur, either an unwound flat ribbon or a narrow fibre with negatively inclined base pairs. The energetics of both types of deformation are similar and existing structures show that at least the flat ribbon form can exist locally under biological conditions.     

Proton nuclear magnetic resonance investigation of the conformation and dynamics in the synthetic deoxyribonucleic acid decamers d(ATATCGATAT) and d(ATATGCATAT)

A variety of one-dimensional proton NMR methods have been used to investigate the properties of two synthetic DNA decamers, d(ATATCGATAT) and d(ATATGCATAT). These results, in conjunction with the results of two-dimensional NMR experiments, permit complete assignment of the base proton resonances. Low-field resonances were assigned by sequential "melting" of the A . T base pairs and by comparison of the spectra of the two decamers. Below 20 degree C spin-lattice relaxation is dominated by through-space dipolar interactions. A substantial isotope effect on the G imino proton relaxation is observed in 75% D2O, confirming the importance of the exchangeable amino protons in the relaxation process. A somewhat smaller isotope effect is observed on the T imino proton relaxation. At elevated temperatures spin-lattice relaxation of the imino protons is due to proton exchange with solvent. Apparent activation energies for exchange vary from 36 kcal/base pair for base pairs (3,8) to 64 kcal/mol for the most interior base pairs (5,6), indicating that disruption of part, or all, of the double helix contributes significantly to the exchange of the imino protons in these decamers. By contrast, single base pair opening events are the major low-temperature pathways for exchange from A X T and G X C base pairs in the more stable higher molecular weight DNA examined in other studies. The temperature dependence of the chemical shifts and line widths of certain aromatic resonances indicates that the interconversion between the helix and coil states is not in fast exchange below the melting temperature, Tm. Within experimental error, no differential melting of base pairs was found in either molecule, and both exhibited melting points Tm = 50-52 degrees C. Spin-spin and spin-lattice relaxation rates of the nonexchangeable protons (TH6, AH8, and AH2) are consistent with values calculated by using an isotropic rotor model with a rotational correlation time of 6 ns and interproton distances appropriate for B-family DNA. The faster decay of AH8 compared with GH8 is attributed to an interaction between the thymine methyl protons and the AH8 protons in adjacent adenines (5'ApT3'). The base protons (AH8, GH8, and TH6) appear to be located close (1.9-2.3 A) to sugar H2',2" protons.(ABSTRACT TRUNCATED AT 400 WORDS)