Two-dimensional nuclear Overhauser enhancement investigation of the solution structure and dynamics of the DNA octamer [d(GGTATACC)]2

The resonances of nearly all 70 of the non-exchangeable protons of the duplex [d(GGTATACC)]2 in aqueous solution are assigned by proton two-dimensional nuclear Overhauser enhancement (2D NOE) spectra obtained in pure absorption phase at 500 MHz. Experimental and theoretical 2D NOE spectra are compared at each mixing time (100, 175, 250 and 400 ms) using two B-DNA structures: a standard B-form and an energy-minimized form. The GG and CC ends of the octamer duplex are well represented by the regular B-DNA structure. But large discrepancies from these models are observed for the 'TATA' box. All 2D NOE data are consistent with nanosecond correlation times, as indicated by non-selective proton spin-lattice relaxation times, but small variations in the correlation time are observed, suggesting that there are some local differences in mobility within the octamer duplex structure in solution.     

Method of determining protein conformations by the two-dimensional nuclear Overhauser enhancement spectroscopy data

A method is suggested to determine the most probable values of the angles phi, psi of the protein backbone by the data on the availability and absence of d connectivities in the two-dimensional nuclear Overhauser enhancement spectra. In view of this, the dependences of the proton-proton distances in dipeptide units of L-amino acid residues on the dihedral angles phi, psi, chi1 are considered and the conformational states of amino acid residues of the proteins with the known spatial structure are analysed statistically. The potentialities of the method are assessed with the aid of model spectral nuclear magnetic resonance (NMR) parameters obtained from the X-ray data for the bovine pancreatic trypsin inhibitor and avian pancreatic polypeptide. It is shown that the developed procedure of structural interpretation of the NMR data allows one to correctly reproduce the local conformation of the protein backbone. The obtained backbone conformation may serve as a starting point to build and refine molecular three-dimensional structure.     

Imino-proton resonances of yeast tRNAPhe studied by two-dimensional nuclear Overhauser enhancement spectroscopy

Application of two-dimensional nuclear Overhauser enhancement (NOE) spectroscopy to yeast tRNAPhe in H2O solution demonstrates that all imino-proton resonances, related to the secondary structure, and nearly all imino proton resonances, originating from the tertiary structure, can be assigned efficiently by this method. The results corroborate the assignments of the imino-proton resonances of this tRNA as established previously by one-dimensional NOE experiments (only the assignment of base pairs G1 X C72 and C2 X G71 should be reversed). The advantages of two-dimensional NOE spectroscopy over one-dimensional NOE spectroscopy for the assignments of imino-proton resonances and the structure elucidation of tRNA are illustrated and discussed. Furthermore, the use of non-exchangeable proton resonances as probes of the molecular structure is explored.     

Solution structure of [d(GTATATAC)]2 via restrained molecular dynamics simulations with nuclear magnetic resonance constraints derived from relaxation matrix analysis of two-dimensional nuclear Overhauser effect experiments

Two-dimensional nuclear Overhauser effect (2D NOE) spectra have been used as the experimental basis for determining the solution structure of the duplex [d(GTATATAC)]2 employing restrained molecular dynamics (rMD) simulations. The MARDIGRAS algorithm has been employed to construct a set of 233 interproton distance constraints via iterative complete relaxation matrix analysis utilizing the peak intensities from the 2D NOE spectra obtained for different mixing times and model structures. The upper and lower bounds for each of the constraints, defining size of a flat-well potential function term used in the rMD simulations, were conservatively chosen as the largest or smallest value calculated by MARDIGRAS. Three different starting models were utilized in several rMD calculations: energy-minimized A-DNA, B-DNA, and a structure containing wrinkled D-DNA in the interior. Considerable effort was made to define the appropriate force constants to be employed with the NOE terms in the AMBER force field, using as criteria the average constraints deviation, the constraints violation energy and the total energy. Of the 233 constraints, one was generated indirectly, but proved to be crucial in defining the structure: the cross-strand A5-H2 A5-H2 distance. As those two protons resonate isochronously for the self-complementary duplex, the distance cannot be determined directly. However, the general pattern of 2D NOE peak intensities, spin-lattice relaxation time (T1) values, and 31P nuclear magnetic resonance spectra lead to use of the A3-H2 A7-H2 distance for A5-H2 A5-H2 as well. Five rMD runs, with different random number seeds, were made for each of the three starting structures with the full distance constraint set. The average structure from all 15 runs and the five-structure averages from each starting structure were all quite similar. Two rMD runs for each starting structure were made with the A5-H2 A5-H2 constraint missing. The average of these six rMD runs revealed differences in structure, compared to that with the full set of constraints, primarily for the middle two base-pairs involving the missing cross-strand constraint but global deviations also were found. Conformational analysis of the resulting structures revealed that the inner four to six base-pairs differed in structure from the termini. Furthermore, an alternating structure was suggested with features alternating for the A-T and T-A steps.     

Local structure of cytochrome c from horse heart in solution. Conformational analysis using data of two-dimensional nuclear Overhauser effect spectroscopy]

Using the earlier suggested method the calculation of the backbone conformations of horse heart cytochrome c in oxidized (ferricytochrome c) and reduced (ferrocytochrome c) states has been performed by the two-dimensional nuclear Overhauser effect spectroscopy data. For both protein forms the secondary structure elements have been revealed and the conformations of the irregular polypeptide chain segments have been analysed. The similarity of the secondary structures of ferri- and ferrocytochrome c in solution was established from the comparison of their conformations. Small differences between the conformations of two molecule forms are shown to be localized within the polypeptide chain fragments situated in the spatial structure near the heme crevice. The comparison of the dihedral phi and psi angles in the calculated conformations of horse cytochrome C with the corresponding characteristics of X-ray structures of tuna ferri- and ferrocytochrome c made for the oxidized and reduced protein forms using the quantitative criteria testifies the similarity of their conformations in solution and crystal. In is shown that the conformational changes of the separate amino acid residues which take place as the result of the "solution-to-crystal" transition occur on the surface fragments of protein globule and do not lead to essential alterations of the secondary molecule structure.     

Conformational analysis of protein side chains using two-dimensional Overhauser nuclear effect spectroscopy]

The method has been proposed to determine the conformations of protein side-chains (dihedral angles chi 1) using two-dimensional nuclear Overhauser effect spectroscopy data. This method is grounded of the algorithm prepared on the basis of joint consideration of proton-proton distance dependences in dipeptide units of L-amino acid residues on the dihedral angles phi, psi and chi 1 with the accounting of the local sterical conditions of the polypeptide chain. The obtained results gave the possibility to bring the different regions of space (phi, psi) of amino acid residues into the line with the specific sets of nuclear Overhauser effect spectral parameters which unambiguously characterize in most cases the conformational states of their side-chains. The method efficiency was displayed on the test calculation with the utilization as the experimental data of the "model" nuclear Overhauser effect contacts derived from the X-ray atomic coordinates of the bovine pancreatic trypsin inhibitor molecule.     

Structure determination of [d(ATATATAUAT)]2 via two-dimensional NOE spectroscopy and molecular dynamics calculations

Proton homonuclear two-dimensional (2D) NOE spectra were obtained for the decamer [d(ATATATAUAT)]2 as a function of mixing time, and proton resonance assignments were made. Quantitative assessment of the 2D NOE cross-peak intensities was used in conjunction with the program MARDIGRAS, which entails a complete relaxation matrix analysis of the 2D NOE peak intensities, to obtain a set of upper and lower bound interproton distance constraints. The analysis with MARDIGRAS was carried out using three initial models: A-DNA, B-DNA and Z-DNA. The distance constraints determined were essentially the same regardless of initial structure. These experimental structural constraints were used with restrained molecular dynamics calculations to determine the solution structure of the decamer. The molecular dynamics program AMBER was run using A-DNA or B-DNA as starting model. The root-mean-square (rms) difference between these two starting models is 0.504 nm. The two starting models were subjected to 22.5 ps of restrained molecular dynamics calculations. The coordinates of the last 10.5 ps of the molecular dynamics runs were averaged to give two final structures. MDA and MDB. The rms difference between these two structures is 0.09 nm, implying convergence of the two molecular dynamics runs. The 2D NOE spectral intensities calculated for the derived structures are in good agreement with experimental spectra, based on sixth-root residual index analysis of intensities. A detailed examination of the structural features suggests that while the decamer is in the B-family of DNA structures, many torsion angle and helical parameters alternate from purine to pyrimidine, with kinks occurring at the U-A steps.     

Solution structure of [d(GCGTATACGC)]2.

The solution structure of the alternating pyrimidine-purine DNA duplex [d(GCGTATACGC)]2 has been determined using two-dimensional nuclear magnetic resonance techniques and distance geometry methods. Backbone distance constraints derived from experimental nuclear Overhauser enhancement and J-coupling torsion angle constraints were required to adequately define the conformation of the inter-residue backbone linkages and to avoid underwinding of the duplex. The distance geometry structures were further refined by back-calculation of the two-dimensional nuclear Overhauser enhancement spectra to correct spin-diffusion distance errors. Fifteen final structures for [d(GCGTATACGC)]2 were generated from the refined experimental distance bounds. These structures all exhibit fully wound B-form geometry with small penalty values (< 1.5 A) against the distance bounds and small pair-wise root-mean-square deviation values (typically 0.6 A to 1.5 A). The final structures exhibit positive base-pair inclination with respect to the helix axis, a marked alternation in rise and twist, and are shorter and wider than classical fiber B-form DNA. The purines were found to adopt a sugar pucker close to the C-2'-endo conformation while pyrimidine sugars exhibited significantly lower pseudorotation phase angles in the C-1'-exo to C-2'-endo range. The minor groove cross-strand steric clashes at pyrimidine-purine steps that would exist in pure B-DNA are attenuated by an increased rise at these steps (and an increased roll angle at TpA steps). Concomitantly the backbone torsion angles of the pyrimidine moieties have larger gamma values, larger epsilon values, and smaller zeta values than the purines. The structures generated by distance geometry methods were also compared with those obtained from restrained molecular dynamics with empirical force-field potentials. The results indicate that the nuclear magnetic resonance/distance geometry approach alone is capable of elucidating most of the salient structural features of double-stranded helical nucleic acids in solution without resorting to empirical energy potentials and without using any structural assumptions from crystallographic data.     

Left-handed helical structure of poly[d(A-C)].poly[d(G-T)] studied by infrared spectroscopy

Infrared spectroscopic studies demonstrate the ability of poly[d(A-C)].poly[d(G-T)] to adopt a Z-type conformation. The Z form of the unmodified polynucleotide is induced by Ni2+ counterions and not by Na+. The B----Z equilibrium is shifted at room temperature, in the presence of 1 Ni2+/nucleotide, by an increase in the concentration of poly[d(A-C)].poly[d(G-T)]. The importance of specific binding of Ni2+ ions on the N7 site of purines in the stabilization of the Z form is also discussed.     

Base tilt of B-form poly[d(G)]-poly[d(C)] and the B- and Z-conformations of poly[d(GC)]-poly[d(GC)] in solution

We have measured the CD, isotropic absorption, and linear dichroism (LD) in the vacuum-uv spectral region for the B-conformations of poly[d(G)]-poly[d(C)] and poly[d(GC)]-poly[d(GC)], and for the Z-conformation of poly[d(GC)]-poly[d(GC)] formed in 70% trifluoroethanol. The reduced dichroism (LD divided by isotropic absorption) for all conformations varied with wavelength, indicating that the bases are not perpendicular to the helix axis. Since the directions of the transition dipoles are known, the inclinations and axes of inclination of each base can be determined from the wavelength dependence of the reduced dichroism spectra. The results indicate that the base normals of the (G + C) polymers in the B- and Z-conformations are tilted at angles greater than 19° with respect to the helix axis. The guanine and cytosine bases have different inclinations, and the tilt axes are not parallel. Therefore, the bases for all the (G + C) polymer conformations studied are buckled and propeller twisted.     

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.     

Conformation of the oligonucleotide d(AAAAAATTTTTT)2 by two-dimensional nuclear Overhauser effect spectroscopy and its relevance to poly(dA).poly(dT)

Conformational analysis from the pattern and intensities of cross-peaks in the two-dimensional nuclear Overhauser effect proton nmr spectra of the homopolymer, poly(dA) · poly(dT), and the analogous oligomer, d(AAAAAATTTTTT)₂, indicate that they both exist in the B-conformation. The conformation of the ApT/TpA junction in the oligomer is significantly different from the rest of the base pairs.     

Novel solution conformation of DNA observed in d(GAATTCGAATTC) by two-dimensional NMR spectroscopy

Resonance assignments of nonexchangeable base and sugar protons of the self-complementary dodecanucleotide d(GAATTCGAATTC) have been obtained by using the two-dimensional Fourier transform NMR methods correlated spectroscopy and nuclear Overhauser effect spectroscopy. Conformational details about the sugar pucker, the glycosidic dihedral angle, and the overall secondary structure of the molecule have been derived from the relative intensities of cross peaks in the two-dimensional NMR spectra in aqueous solution. It is observed that d(GAATTCGAATTC) assumes a novel double-helical structure. The solution conformations of the two complementary strands are identical, unlike those observed in a related sequence in the solid state. Most of the five-membered sugar rings adopt an unusual O1'-endo geometry. All the glycosidic dihedral angles are in the anti domain. The AATT segments A2-T5 and A8-T11 show better stacking compared to the rest of the molecule. These features fit into a right-handed DNA model for the above two segments, with the sugar geometries different from the conventional ones. There are important structural variations in the central TCG portion, which is known to show preferences for DNase I activity, and between G1-A2 and G7-A8, which are cleavage points in the EcoRI recognition sequence. The sugar puckers for G1 and G7 are significantly different from the rest of the molecule. Further, in the three segments mentioned above, the sugar phosphate geometry is such that the distances between protons on adjacent nucleotides are much larger than those expected for a right-handed DNA. We suggest that such crevices in the DNA structure may act as "hot points" in initiation of protein recognition.     

Conformation of the third domain of turkey ovomucoid in solution. Structural analysis by two-dimensional Overhauser nuclear effect spectroscopy]

The conformations of a polypeptide chain of turkey ovomucoid third domain and its modified form with split reactive site peptide bond Leu-18--Glu-19 have been determined by the literary two-dimensional nuclear Overhauser effect spectroscopy data using an earlier suggested method. It has been found that the polypeptide domain backbone contains an alpha-helical fragment (residues 32-47), five segments having extended conformation (1-5, 11-17, 19-25, 29-31, 48-50) and beta-turn type 1 (26-29). Segments 23-26, 28-31 and 50-51 form an antiparallel beta-structure. Conformational states of the residues entering irregular domain segments have been analysed. Splitting of the reactive site peptide bond Leu-18--Glu-19 is shown to cause insignificant changes in the conformations of a number of amino acid residues except for Val-6 and Asp-7 ones which undergo essential conformational alterations. The conformations of domain in solution and of japanese quail ovomucoid third domain in crystal have been compared. The root-mean-square deviations for phi and psi angles indicate their high similarity. The conformations of turkey ovomucoid third domain and proteinase inhibitor BUSI IIA in solution have been analysed. In spite of moderate (50%) homology of primary structures, some 75% of amino acid residues are shown to have close conformational phi and psi parameters.     

Four-dimensional 13C/13C-edited nuclear Overhauser enhancement spectroscopy of a protein in solution: application to interleukin 1 beta

A four-dimensional 13C/13C-edited NOESY experiment is described which dramatically improves the resolution of protein NMR spectra and enables the straightforward assignment of nuclear Overhauser effects involving aliphatic and/or aromatic protons in larger proteins. The experiment is demonstrated for uniformly (greater than 95%) 13C-labeled interleukin 1 beta, a protein of 153 residues and 17.4 kDa, which plays a key role in the immune response. NOEs between aliphatic and/or aromatic protons are first spread out into a third dimension by the 13C chemical shift of the carbon atom attached to the originating proton and subsequently into a fourth dimension by the 13C chemical shift of the carbon atom attached to the destination proton. Thus, each NOE cross peak is labeled by four chemical shifts. By this means, ambiguities in the assignment of NOEs that arise from chemical shift overlap and degeneracy are completely removed. Further, NOEs between protons with the same chemical shifts can readily be detected providing their attached carbon atoms have different 13C chemical shifts. The design of the pulse sequence requires special care to minimize the level of artifacts arising from undesired coherence transfer pathways, and in particular those associated with "diagonal" peaks which correspond to magnetization that has not been transferred from one proton to another.(ABSTRACT TRUNCATED AT 250 WORDS)     

Solution structure of [d(A-T)5]2 via complete relaxation matrix analysis of two-dimensional nuclear Overhauser effect spectra and molecular mechanics calculations: evidence for a hydration tunnel

Pure absorption phase proton two-dimensional nuclear Overhauser effect (2D NOE) spectra at 500 MHz have been obtained for [d(5'ATATATATAT3')]2 in deuterium oxide solution at several mixing times. The 100 nonexchangeable proton resonances have been assigned. The experimental 2D NOE spectra were compared with theoretical spectra calculated by using the complete relaxation matrix analysis method [Keepers, J. W., & James, T. L. (1984) J. Magn. Reson. 57, 404-426] and x-ray diffraction determined molecular coordinates of A, B, alternating B, left-handed B, C, D, and wrinkled D forms of DNA and of energy-minimized structures calculated from the most promising X-ray crystal structures by using the molecular mechanics program AMBER, in which all hydrogens, counterions, and hydration water molecules were included. The analysis of all features of the 2D NOE spectra played an important role in extracting the promising structures, and it was concluded that the wrinkled D form yields the best fit for the 2D NOE data of the A-T decamer. The molecular mechanics calculation indicated that this model structure, whose minor groove is comparatively deep and narrow, may be energetically more stable than the B form for alternating d(A-T) DNA. Interesting features of the structure include possible intra- and interchain sugar-phosphate attractions and a hydration tunnel inside the minor groove capable of accommodating three types of water molecules that aid in helix stabilization via hydrogen bonding. Counterions (sodium) serve to reduce interchain phosphate-phosphate repulsive effects.     

Determination of interproton distances in peptides by two-dimensional nuclear Overhauser effect spectroscopy (NOESY). Conformation of a cyclic analog of substance P in a solution

Quantitative method is developed for evaluation interproton distances in peptides in solution. The method is based on the measurement of the relative intensities of the cross-peaks in the pure-phase absorption NOESY spectra. The ratios of the cross-peak intensities IN alpha/I alpha N and INN/I alpha N enable to determine the corresponding interproton distances dN alpha, d alpha N and dNN for several amino acid residues. These distances can be used to estimate other distances with cross-peaks in NOESY spectra. As example, the interproton distances are determined in a cyclic hexapeptide, namely cyclic analogue of substance P: cyclo [H-Glu-Phe-Phe-Gly-Leu-Met-NH(CH2)3-NH-]. The spatial structure of the molecule in dimethylsulphoxide solution is established.     

A two-dimensional nuclear Overhauser enhancement (2D NOE) experiment for the elucidation of complete proton-proton cross-relaxation networks in biological macromolecules

The recently developed technique of two-dimensional (2D) cross-relaxation spectroscopy is utilized for systematic measurements of selective nuclear Overhauser enhancements (NOE) in the high resolution ¹H nuclear magnetic resonance (NMR) spectra of biological macromolecules in solution. Compared to conventional one-dimensional NOE studies, the 2D NOE experiment has the principal advantage that it avoids detrimental effects arising from the limited selectivity of preirradiation in crowded spectral regions. Furthermore, it yields with a single instrument setting a complete network of NOE's between all the protons in the macromolecule. The resulting information on intramolecular proton-proton distances provides a new avenue for studies of the spatial structures of biopolymers.     

Nitrogen mustard fixes the Z-conformation in poly[d(G-C)]poly[d(G-C)] and DNA]

The reactions of poly(dG-dC).poly(dG-dC) and (dG-dC)10 insert in the plasmid pGC20 with N-methyl-bis(2-chloroethyl)-amine (nitrogen mustard, HN-2) have been studied. It is shown that nitrogen mustard does not induce the B----Z transition in poly(dG-dC).poly(dG-dC), but produces fixation of the polynucleotide Z-conformation once this exists. In the case of pGC20 plasmid DNA, nitrogen mustard also fixes Z-form of the (dG-dC)-insert. The rate constant of the reaction of nitrogen mustard with guanine in the polynucleotide (k = 9,0.10(-3) min-1) is about one-third of that for the fixation of Z-form of the (dG-dC)-insert in the plasmid (k1 = 2,8.10(-2) min-1) which is attributed to a greater rate of formation of diguanyl derivative in the opposite DNA chains. It is suggested that nitrogen mustard is capable of fixing the Z-form DNA not only in vitro, but also in vivo.     

From determination of amino acid residue conformation to reconstruction of the spatial structure of proteins (from the data of nuclear Overhauser enhancement spectroscopy

A new approach to the calculation of the spatial protein structure based on the joint utilization of the theoretical conformational analysis method and nuclear Overhauser enhancement (NOE) spectroscopy data is proposed and verified. The quality in determining various molecule structural parameters is estimated in terms of the expected NOE spectral parameters derived from the X-ray analysis data of the avian pancreatic polypeptide. The proposed approach is shown to correctly determine such structural parameters of protein molecules as local amino acid residue conformations, reciprocal spatial orientation of the C alpha atoms neighbouring along amino acid sequence and reapproached segments of the polypeptide chain. Spatially remote molecule fragments are mainly responsible for the error in determining structural parameters.