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.     

Solution structure of the EcoRI DNA sequence: refinement of NMR-derived distance geometry structures by NOESY spectrum back-calculations

The solution structure of the self-complementary DNA duplex [d(CGCGAATTCGCG)]2, which contains the EcoRI restriction site sequence GAATTC at the center, has been studied by two-dimensional nuclear magnetic resonance spectroscopy. Time-dependent nuclear Overhauser effect spectra were used to obtain the initial cross-relaxation rates between 155 pairs of protons. These initial cross-relaxation rates were converted into interproton distances and entered into a distance (bounds) matrix. A distance geometry algorithm (DSPACE) was used to create embedded starting structures and to refine these structures until they showed good agreement with the distance matrix; symmetry constraints were included in the refinement procedure, making the two strands in the refined distance geometry structures virtually identical and significantly improving the agreement with the distance matrix. The NOESY spectrum for one of these distance geometry structures was then calculated from the explicit coordinates by numerically integrating all the z-magnetization transfer pathways among neighboring protons within a specified radius. Distances in this distance geometry structure that did not agree with the experimental NOESY time course were then adjusted accordingly. This process was iterated until a good agreement between calculated and experimental NOESY spectra was reached. The final structure, which generates good agreement with the experimental NOESY spectrum, displays kinks at the C3-G4 base step and at the A6-T7 base step that appear to be similar to those reported for the EcoRI restriction site DNA bound to its endonuclease. The solution structure is not the same as the crystal structure of this DNA duplex.     

Solution structure of the TnAn DNA duplex GCCGTTAACGCG containing the HpaI restriction site.

The solution structure of the self-complementary DNA duplex [d(GCCGTTAACGGC)]2, which contains the HpaI restriction site GTTAAC, has been elucidated by two-dimensional NMR, distance geometry (DG), and NOE back-calculation methods. Initial distance constraints were determined by polynomial fitting the two-spin initial NOE rates; backbone constraints from NOE and J-coupling observations (Kim et al., 1992) were included. RMSDs between initial-distance-refined structures derived from random-embedded DG, A-DNA, and B-DNA starting structures were all in the range 0.5-1.0 A, indicating good convergence properties of the algorithm, regardless of the starting structure. A semiautomatic back-calculation refinement procedure was developed and used to generate more refined structures for which the BKCALC-simulated NOE volumes matched the experimental data. The six final structures refined from various starting structures exhibit very good agreement with the experimental data (R values = 0.18) and converge well to within 0.8-A RMSD differences for the central 8 base pairs. The torsion and pseudorotation phase angles were found to be well determined by the data, and the local helical parameters for each base step converged quite well. The final structures show that the central T6-A7 step is somewhat underwound (twist angle ca. 29 degrees), with a large negative cup and a normal (wide) minor groove width, while the T5-T6 and A7-A8 steps have a partially narrowed minor groove.     

2'-deoxyribonolactone lesion in DNA: refined solution structure determined by nuclear magnetic resonance and molecular modeling

The solution conformation of the DNA duplex d(C1G2C3A4C5L6C7A8C9G10C11).d(G12C13G14T15G16T17G18T19G20C21G22 ) containing the 2'-deoxyribonolactone lesion (L6) in the middle of the sequence has been investigated by NMR spectroscopy and restrained molecular dynamics calculations. Interproton distances have been obtained by complete relaxation matrix analysis of the NOESY cross-peak intensities. These distances, along with torsion angles for sugar rings and additional data derived from canonical A- and B-DNA, have been used for structure refinement by restrained molecular dynamics (rMD). Six rMD simulations have been carried out starting from both regular A- and B-DNA forms. The pairwise rms deviations calculated for each refined structure are <1 A, indicating convergence to essentially the same geometry. The accuracy of the rMD structures has been assessed by complete relaxation matrix back-calculation. The average sixth-root residual index (Rx = 0.052 +/- 0.003) indicated that a good fit between experimental and calculated NOESY spectra has been achieved. Detailed analysis revealed a right-handed DNA conformation for the duplex in which both the T17 nucleotide opposite the abasic site and the lactone ring are located inside the helix. No kinking is observed for this molecule, even at the abasic site step. This structure is compared to that of the oligonucleotide with the identical sequence containing the stable tetrahydrofuran abasic site analogue that we reported previously [Coppel, Y., Berthet, N., Coulombeau, C., Coulombeau, Ce., Garcia, J., and Lhomme, J. (1997) Biochemistry 36, 4817-4830].     

Solution conformation of the (+)-trans-anti-benzo[g]chrysene-dA adduct opposite dT in a DNA duplex.

The solution structure of the adduct derived from the covalent bonding of the fjord region (+)-(11S, 12R, 13R, 14S) stereoisomer of anti -11,12-dihydroxy-13,14-epoxy-11,12,13, 14-tetrahydrobenzo[g]chrysene, (+)- anti -B[g]CDE, to the exocyclic N(6)amino group of the adenine residue dA6, (designated (+)- trans-anti -(B[g]C)dA6), positioned opposite a thymine residue dT17 in the DNA sequence context d(C1-T2-C3-T4-C5-(B[g]C)A6-C7-T8-T9-C10-C11). d(G12-G13-A14-A15-G16-T17-G18-A19-G20++ +-A21-G22) (designated (B[g]C)dA. dT 11-mer duplex), has been studied using structural information derived from NMR data in combination with molecular dynamics (MD) calculations. The solution structure of the (+)- trans-anti -(B[g]C)dA.dT 11-mer duplex has been determined using an MD protocol where both interproton distance and dihedral angle restraints deduced from NOESY and COSY spectra are used during the refinement process, followed by additional relaxation matrix refinement to the observed NOESY intensities to account for spin diffusion effects. The results established that the covalently attached benzo[g]chrysene ring intercalates into the DNA helix directed towards the 5'-side of the modified strand and stacks predominantly with dT17 when intercalated between dC5.dG18 and (B[g]C)dA6.dT17 base-pairs. All base-pairs, including the modified (B[g]C)dA6.dT17 base-pair, are aligned through Watson-Crick pairing as in normal B -DNA. In addition, the potential strain associated with the highly sterically hindered fjord region of the aromatic portion of the benzo[g]chrysenyl ring is relieved through the adoption of a non-planar, propeller-like geometry within the chrysenyl ring system. This conformation shares common structural features with the related (+)- trans-anti -(B[c]Ph)dA adduct in the identical base sequence context, derived from the fjord region (+)-(1S,2R,3R,4S)-3, 4-dihydroxy-1,2-epoxy-1,2,3,4-tetrahydrobenzo[c]phenanthrene stereoisomer, in which intercalation is also observed towards the 5'-side of the modified dA6.dT17 base-pair.     

Comparison of the accuracy of protein solution structures derived from conventional and network-edited NOESY data.

Network-editing experiments are variants of the basic NOESY experiment that allow more accurate direct measurement of interproton distances in macromolecules by defeating specific spin-diffusion pathways. Two network-editing approaches, block-decoupled NOESY and complementary-block-decoupled-NOESY, were applied as three-dimensional, heteronuclear-edited experiments to distance measurement in a small protein, turkey ovomucoid third domain (OMTKY3). Two-hundred and twelve of the original 655 distance constraints observed in this molecule (Krezel AM et al., 1994, J Mol Biol 242:203-214) were improved by their replacement by distances derived from network-edited spectra, and distance geometry/simulated annealing solution structure calculations were performed from both the unimproved and improved distance sets. The resulting two families of structures were found to differ significantly, the most important differences being the hinge angle of a beta-turn and an expansion of the sampled conformation space in the region of the reactive-site loop. The structures calculated from network-editing data are interpreted as a more accurate model of the solution conformation of OMTKY3.     

Extrahelical adenosine stacks into right-handed DNA: solution conformation of the d(C-G-C-A-G-A-G-C-T-C-G-C-G) duplex deduced from distance geometry analysis of nuclear Overhauser effect spectra

This paper reports on features of the three-dimensional structure of the d(C-G-C-A-G-A-G-C-T-C-G-C-G) self-complementary duplex (designated adenosine 13-mer), which contains symmetrical extrahelical adenosines in the interior of the helix. The majority of the protons have been assigned from two-dimensional nuclear Overhauser effect (NOESY) spectra of the adenosine 13-mer in H2O and D2O solution. The measurement of NOESY cross-peak volume integrals as a function of mixing time has yielded a set of 96 short (less than 4.5-A) proton-proton distances defined by lower and upper bounds, which have served as input parameters for a distance geometry analysis of one symmetric half of the adenosine 13-mer duplex. We demonstrate that the extrahelical adenosine stacks into the duplex for all refined structures without disruption of base pairing on either side of the modification site. The distance geometry refinement yields two classes of conformations consistent with distance measurements but which differ in orientation of the stacked extrahelical adenosine at the modification site.     

Solution structures of a DNA dodecamer duplex with and without a cisplatin 1,2-d(GG) intrastrand cross-link: comparison with the same DNA duplex containing an oxaliplatin 1,2-d(GG) intrastrand cross-link

Proteins that discriminate between cisplatin-DNA adducts and oxaliplatin-DNA adducts are thought to be responsible for the differences in tumor range, toxicity, and mutagenicity of these two important chemotherapeutic agents. However, the structural basis for differential protein recognition of these adducts has not been determined and could be important for the design of more effective platinum anticancer agents. We have determined high-resolution NMR structures for cisplatin-GG and undamaged DNA dodecamers in the AGGC sequence context and have compared these structures with the oxaliplatin-GG structure in the same sequence context determined previously in our laboratory. This structural study allows the first direct comparison of cisplatin-GG DNA and oxaliplatin-GG DNA solution structures referenced to undamaged DNA in the same sequence context. Non-hydrogen atom rmsds of 0.81 and 1.21 were determined for the 15 lowest-energy structures for cisplatin-GG DNA and undamaged DNA, respectively, indicating good structural convergence. The theoretical NOESY spectra obtained by back-calculation from the final average structures showed excellent agreement with the experimental data, indicating that the final structures are consistent with the NMR data. Several significant conformational differences were observed between the cisplatin-GG adduct and the oxaliplatin-GG adduct, including buckle at the 5' G6.C19 base pair, opening at the 3' G7.C18 base pair, twist at the A5G6.T20C19 base pair step, slide, twist, and roll at the G6G7.C19C18 base pair step, slide at the G7C8.C18G17 base pair step, G6G7 dihedral angle, and overall bend angle. We hypothesize that these conformational differences may be related to the ability of various DNA repair proteins, DNA binding proteins, and DNA polymerases to discriminate between cisplatin-GG and oxaliplatin-GG adducts.     

Spatial structure of (1-36)bacterioopsin solubilized in a methanol-chloroform mixture with sodium dodecylsulfate micelles]

Spatial structures of proteolytic segment A (sA) of bacterioopsin of Halobacterium halobium (residues 1-36) solubilized in the mixture of methanol-chloroform (1:1), 0.1 M LiClO4 or in perdeuteriated sodium dodecyl sulfate (SDS) micelles, were determined by 2D 1H-NMR techniques. Most of the resonances in 1H-NMR spectra of fragment A were assigned using DQF-COSY, TOCSY and NOESY spectra. Deuterium exchange rates for amide protons were measured in series of NOESY spectra. 324 and 400 NOESY cross-peak volumes were measured in NOESY spectra of sA in mixture of organic solvents and SDS micelles, respectively. The sA structure was determined by local structure analysis, distance geometry calculation with program DIANA and systematic search for energetically allowed side chain rotamers consistent with NOESY cross-peak volumes. The structures of sA are similar in both milieus. These structures have the right-handed alpha-helical region from Pro-8 to Met-32 with root mean square deviation (RMSD) of 0.25 A between back bone heavy atoms and fit well with Pro-8 to Met-32 alpha-helical region in electron cryo-microscopy (ECM) model of bacteriorhodopsin [4]. The C-terminal region Gly-33-Asp-36 is disordered in both milieus, while N-terminal region Ala-2-Gly-6 in organic solvents has a fixed structure (RMSD of 0.25 A) stabilized by the Thr-5 NH...O=C Gln-3 and Ile-4 NH...O = C Ala-2 hydrogen bonds. This region of sA in SDS micelles has disordered structure with RMSD of 1.44 A for back bone heavy atoms. Torsion angles chi 1 of sA were unequivocally determined for 72% of side chains in the alpha-helical region and are identical in both milieus.     

NMR solution structure of the catalytic fragment of human fibroblast collagenase complexed with a sulfonamide derivative of a hydroxamic acid compound.

The solution structure of the catalytic fragment of human fibroblast collagenase (MMP-1) complexed with a sulfonamide derivative of a hydroxamic acid compound (CGS-27023A) has been determined using two-dimensional and three-dimensional heteronuclear NMR spectroscopy. The solution structure of the complex was calculated by means of hybrid distance geometry-simulated annealing using a combination of experimental NMR restraints obtained from the previous refinement of the inhibitor-free MMP-1 (1) and recent restraints for the MMP-1:CGS-27023A complex. The hydroxamic acid moiety of CGS-27023A was found to chelate to the "right" of the catalytic zinc where the p-methoxyphenyl sits in the S1' active-site pocket, the isopropyl group is in contact with H83 and N80, and the pyridine ring is solvent exposed. The sulfonyl oxygens are in hydrogen-bonding distance to the backbone NHs of L81 and A82. This is similar to the conformation determined by NMR of the inhibitor bound to stromelysin (2, 3). A total of 48 distance restraints were observed between MMP-1 and CGS-27023A from 3D 13C-edited/12C-filtered NOESY and 3D 15N-edited NOESY experiments. An additional 18 intramolecular restraints were observed for CGS-27023A from a 2D 12C-filtered NOESY experiment. A minimal set of NMR experiments in combination with the free MMP-1 assignments were used to assign the MMP-1 (1)H, 13C, and 15N resonances in the MMP-1:CGS-27023A complex. The assignments of CGS-27023A in the complex were obtained from 2D 12C-filtered NOESY and 2D 12C-filtered TOCSY experiments.     

Synthesis, structure, and reactivity of monofunctional platinum(II) and palladium(II) complexes containing the sterically hindered ligand 6-(methylpyridin-2-yl)acetate

Three complexes containing the novel, sterically hindered ligand 6-(methylpyridin-2-yl)acetate (PICAC) have been synthesized and characterized: [Pt(NH3)2(PICAC-N,O)]NO3 (1), [Pt(en)(PICAC-N,O)]NO3 (2), and [Pd(en)(PICAC-N,O)]NO3 (3) (en = ethane-1,2-diamine). The crystal structures of 2 and 3 have been determined. The two complexes are isostructural and exhibit a mixed [N3O] coordination. In both cases, PICAC forms a sterically crowded six-membered chelate. Signal multiplicities in 1H NMR spectra of 1-3 indicate that the N,O chelates are conformationally rigid on the NMR timescale as a result of the steric bulk of the pyridine derivative. Complex 2 undergoes facile ring opening in 0.1M NaCl solution at neutral pH, resulting in a zwitterionic species in which carboxylate oxygen has been replaced with chloride. The complex was identified by X-ray crystallography as [PtCl(en)(PICAC-N)] x H2O (4), which contains a "dangling" carboxylate group. In 4, the pyridine moiety adopts an almost perpendicular orientation relative to the platinum coordination plane. Likewise, complex 2 reacts rapidly with 5'-guanosine monophosphate (5'-GMP) to form the monofunctional adduct [Pt(en)(PICAC)(5'-GMP)] (5) (NMR, 25 degrees C, t(1/2) approximately 24 min). 2-D nuclear Overhauser enhancement spectroscopy (NOESY) and double quantum-filtered correlated spectroscopy (dqf-COSY) experiments (500 MHz) and variable temperature NMR spectroscopy confirm that adduct 5 exists as a 1:1 mixture of rotamers in solution as a result of the mutual repulsion between the cis-oriented pyridine and guanine bases. While 2 readily reacts with DNA nitrogen, its monofunctional adducts show no significant effect on the conformation of native DNA. Circular dichroism (CD) spectra recorded of platinum-modified calf-thymus DNA suggest that the structural damage produced by complex 2 does not mimic that produced by the clinical agent. Both the unusual reactivity and the inability to induce cisplatin-like DNA conformational changes are proposed to be responsible for the marginal biological activity of the new complexes.     

Conformation of [Cd7]-metallothionein-2 from rat liver in aqueous solution determined by nuclear magnetic resonance spectroscopy

The three-dimensional structure of [Cd7]-metallothionein-2 from rat liver was determined in aqueous solution, using nuclear magnetic resonance spectrometry and distance geometry calculations. The experimental data provided proton-proton distance constraints from measurements of nuclear Overhauser effects, constraints on the geometry of the metal-cysteine clusters determined by heteronuclear correlation spectroscopy, and dihedral angle constraints derived from both coupling constants and nuclear Overhauser effects. The structure calculations were performed with the program DISMAN. As in previous studies with rabbit liver metallothionein-2a, the structure calculations were performed separately for the alpha and beta-domains containing the 4 and 3-metal clusters, respectively, since no interdomain constraints were found. For both domains, the global polypeptide fold, the location of polypeptide secondary structure elements, the architecture of the metal-sulfur cluster and the local chirality of the metal co-ordination are very similar to the solution structure of rabbit metallothionein-2a, but show considerable difference relative to the crystal structure of rat metallothionein-2.     

Three-dimensional solution structure of Ca(2+)-loaded porcine calbindin D9k determined by nuclear magnetic resonance spectroscopy.

The three-dimensional solution structure of native, intact porcine calbindin D9k has been determined by distance geometry and restrained molecular dynamics calculations using distance and dihedral angle constraints obtained from 1H NMR spectroscopy. The protein has a well-defined global fold consisting of four helices oriented in a pairwise antiparallel manner such that two pairs of helix-loop-helix motifs (EF-hands) are joined by a linker segment. The two EF-hands are further coupled through a short beta-type interaction between the two Ca(2+)-binding loops. Overall, the structure is very similar to that of the highly homologous native, minor A form of bovine calbindin D9k determined by X-ray crystallography [Szebenyi, D. M. E., & Moffat, K. (1986) J. Biol. Chem. 261, 8761-8776]. A model structure built from the bovine calbindin D9k crystal structure shows several deviations larger than 2 A from the experimental distance constraints for the porcine protein. These structural differences are efficiently removed by subjecting the model structure to the experimental distance and dihedral angle constraints in a restrained molecular dynamics protocol, thereby generating a model that is very similar to the refined distance geometry derived structures. The N-terminal residues of the intact protein that are absent in the minor A form appear to be highly flexible and do not influence the structure of other regions of the protein. This result is important because it validates the conclusions drawn from the wide range of studies that have been carried out on minor A forms rather than the intact calbindin D9k.     

The solution structure of a [3Fe-4S] ferredoxin: oxidised ferredoxin II from Desulfovibrio gigas

The use of standard 2D NMR experiments in combination with 1D NOE experiments allowed the assignment of 51 of the 58 spin systems of oxidised [3Fe-4S] ferredoxin isolated from Desulfovibrio gigas. The NMR solution structure was determined using data from 1D NOE and 2D NOESY spectra, as distance constraints, and information from the X-ray structure for the spin systems not detected by NMR in torsion angle dynamics calculations to produce a family of 15 low target function structures. The quality of the NMR family, as judged by the backbone r.m.s.d. values, was good (0.80?Å), with the majority of φ/ψ angles falling within the allowed region of the Ramachandran plot. A comparison with the X-ray structure indicated that the overall global fold is very similar in solution and in the solid state. The determination of the solution structure of ferredoxin II (FdII) in the oxidised state (FdII_ox) opens the way for the determination of the solution structure of the redox intermediate state of FdII (FdII_int), for which no X-ray structure is available.     

Solution conformation on bovine growth hormone releasing factor by 1H NMR and molecular modeling.

The structure of bovine growth hormone releasing factor (bGHRF) consisting of 44 amino acids has been studied in CD and 1H nuclear magnetic resonance (NMR) spectroscopy in conjunction with molecular modeling. Since bGHRF does not have an ordered structure in water alone, a 30% 2,2,2-trifluoroethanol (TFE) aqueous solvent was used to induce considerable alpha-helical structures, which corresponds to a helical content of approximately 62% as determined by circular dichroism (CD). The secondary structure was obtained from nuclear Overhauser enhancement and 3J(HN alpha) coupling constant in 30% TFE solution. Three-dimensional structures consistent with NMR data were generated by using distance geometry calculation. A set of 267 interproton distances derived from nuclear Overhauser effect correlation spectroscopy (NOESY) experiments and coupling constants were used. From the initial random conformations, 50 distance geometry structures with minimal violations were selected for further refinement. The 14 best structures were obtained after simulated annealing calculation with energy minimization. The structure of bGHRF in 30% TFE solution was characterized by one alpha-helix (residues 8-19), two poorly constrained helices (residues 23-27 and residues 31-34) and a beta I(III)-turn fragment (residues 20-23; phi(i+1) = -53.1 degrees, psi(i+1) = -19.6 degrees, phi(i+2) = -59.9 degrees, psi(i+2) = -20.6 degrees) connected by the segments of less defined structures in N-terminal and omega-shaped flexible C-terminal determined from NOESY cross peaks between helical segment (residues 14-18) and tail fragment (residues 42-44). The obtained structure will play an important role toward the understanding of the structural and functional role of the GHRF.     

Determination of the structure of [Nle7]-endothelin by 1H NMR

[Nle7]-endothelin was synthesized and studied by 1H NMR and distance geometry calculations. The NMR study was performed first in DMSO-d6 and then in 50% acetonitrile/water since this peptide aggregates in pure water. In both cases, all spin systems were identified and assigned with the aid of two-dimensional spectroscopy (2D): COSY (for scalar couplings) and NOESY (for dipolar couplings). On the basis of the acetonitrile/water NMR parameters, and using the DISGEO program, a three-dimensional structure of [Nle7]-endothelin is proposed and discussed.     

Determination of a high precision structure of a novel protein, Linum usitatissimum trypsin inhibitor (LUTI), using computer-aided assignment of NOESY cross-peaks

The solution structure of a novel 69 residue proteinase inhibitor, Linum usitatissimum trypsin inhibitor (LUTI), was determined using a method based on computer aided assignment of nuclear Overhauser enhancement spectroscopy (NOESY) data. The approach applied uses the program NOAH/DYANA for automatic assignment of NOESY cross-peaks. Calculations were carried out using two unassigned NOESY peak lists and a set of determined dihedral angle restraints. In addition, hydrogen bonds involving amide protons were identified during calculations using geometrical criteria and values of HN temperature coefficients. Stereospecific assignment of beta-methylene protons was carried out using a standard procedure based on nuclear Overhauser enhancement intensities and 3J(alpha)(beta) coupling constants. Further stereospecific assignment of methylene protons and diastereotopic methyl groups were established upon structure-based method available in the program GLOMSA and chemical shift calculations. The applied algorithm allowed us to assign 1968 out of 2164 peaks (91%) derived from NOESY spectra recorded in H2O and 2H2O. The final experimental data input consisted of 1609 interproton distance restraints, 88 restraints for 44 hydrogen bonds, 63 torsion angle restraints and 32 stereospecifically assigned methylene proton pairs and methyl groups. The algorithm allowed the calculation of a high precision protein structure without the laborious manual assignment of NOESY cross-peaks. For the 20 best conformers selected out of 40 refined ones in the program CNS, the calculated average pairwise rmsd values for residues 3 to 69 were 0.38 A (backbone atoms) and 1.02 A (all heavy atoms). The three-dimensional LUTI structure consists of a mixed parallel and antiparallel beta-sheet, a single alpha-helix and shows the fold of the potato 1 family of proteinase inhibitors. Compared to known structures of the family, LUTI contains Arg and Trp residues at positions P6' and P8', respectively, instead of two Arg residues, involved in the proteinase binding loop stabilization. A consequence of the ArgTrp substitution at P8' is a slightly more compact conformation of the loop relative to the protein core.     

Structure determination of [Arg8]vasopressin methylenedithioether in dimethylsulfoxide using NMR.

The structure of [Arg8]vasopressin methylenedithioether ([AVP]CH2) has been determined in dimethylsulfoxide-d6. Two-dimensional DQF-COSY and NOESY spectra were measured and used to derive angle and distance constraints for restrained molecular dynamics (MD) calculations. In the MD trajectory, two types of beta-turn structure were found in the region from Tyr2 to Asn5, suggesting an equilibrium between type-I and type-II' beta-turn structures. When Halpha chemical shifts were used as an additional constraint, the type-I turn was favoured. To validate this result, an independent energy minimization procedure was used, using differences between calculated and observed chemical shifts. The two approaches gave essentially identical results. It is therefore concluded that the type-I turn predominates in solution. Analysis of calculated chemical shift contributions suggests that the beta-turn structure found in AVP is well preserved in [AVP]CH2, although the pressin ring size is expanded.     

Solution structure of [d(ATGAGCGAATA)]2. Adjacent G:A mismatches stabilized by cross-strand base-stacking and BII phosphate groups.

The solution structure of a rather unusual B-form duplex [d(ATGAGCGAATA)]2 has been determined using two-dimensional nuclear magnetic resonance (2D-NMR) and distance geometry methods. This sequence forms a stable ten base-pair B-form duplex with 3' overhangs and two pairs of adjacent G:A mismatches paired via a sheared hydrogen-bonding scheme. All non-exchangeable protons, including the stereo-specific H-5'S/H-5'R of the 3G and 7G residues, were assigned by 2D-NMR. The phosphorus spectrum was assigned using heteronuclear correlation with H-3' and H-4' reasonances. The complete assignments reveal several unusual nuclear Overhauser enhancements (NOEs) and unusual chemical shifts for the neighboring G:A mismatch pairs and their adjacent nucleotides. Inter-proton distances were derived from time-dependent NOEs and used to generate initial structures, which were further refined by iterative back-calculation of the two-dimensional nuclear Overhauser enhancement spectra; 22 final structures were calculated from the refined distance bounds. All these final structures exhibit fully wound helical structures with small penalty values against the refined distance bounds and small pair-wise root-mean-square deviation values (typically 0.5 A to 0.9 A). The two helical strands exchange base stacking at both of the two G:A mismatch sites, resulting in base stacking down each side rather than down each strand of the twisted duplex. Very large twist angles (77 degrees) were found at the G:A mismatch steps. All the final structures were found to have BII phosphate conformations at the adjacent G:A mismatch sites, consistent with observed downfield 31P chemical shifts and Monte-Carlo conformational search results. Our results support the hypothesis that 31P chemical shifts are related to backbone torsion angles. These BII phosphate conformations in the adjacent G:A mismatch step suggest that hydrogen bonding of the G:A pair G-NH2 to a nearby phosphate oxygen atom is unlikely. The unusual structure of the duplex may be stabilized by strong interstrand base stacking as well as intrastrand stacking, as indicated by excellent base overlap within the mismatch stacks.     

Raman spectra of single crystals of r(GCG)d(CGC) and d(CCCCGGGG) as models for A DNA, their structure transitions in aqueous solution, and comparison with double-helical poly(dG).poly(dC)

The self-complementary oligonucleotides [r(CGC)d(CGC)]2 and [d(CCCCGGGG)]2 in single-crystal and solution forms have been investigated by Raman spectroscopy. Comparison of the Raman spectra with results of single-crystal X-ray diffraction and with data from polynucleotides permits the identification of a number of Raman frequencies diagnostic of the A-helix structure for GC sequences. The guanine ring frequency characteristic of C3'-endo pucker and anti base orientation is assigned at 668 +/- 2 cm-1 for both dG and rG residues of the DNA/RNA hybrid [r(GCG)d(CGC)]2. The A-helix backbone of crystalline [r(GCG)d(CGC)]2 is altered slightly in the aqueous structure, consistent with the conversion of at least two residues to the C2'-endo/anti conformation. For crystalline [d(CCCCGGGG)]2, the Raman and X-ray data indicate nucleosides of alternating 2'-endo-3'-endo pucker sandwiched between terminal and penultimate pairs of C3'-endo pucker. The A-A-B-A-B-A-A-A backbone of the crystalline octamer is converted completely to a B-DNA fragment in aqueous solution with Raman markers characteristic of C2'-endo/anti-G (682 +/- 2) and the B backbone (826 +/- 2 cm-1). In the case of poly(dG).poly(dC), considerable structural variability is detected. A 4% solution of the duplex is largely A DNA, but a 2% solution is predominantly B DNA. On the other hand, an oriented fiber drawn at 75% relative humidity reveals Raman markers characteristic of both A DNA and a modified B DNA, not unlike the [d-(CCCCGGGG)]2 crystal. A comparison of Raman and CD spectra of the aqueous [d(CCCCGGGG)]2 and poly(dG).poly(dC) structures suggests the need for caution in the interpretation of CD data from G clusters in DNA.