Determination of the three-dimensional solution structure of barnase using nuclear magnetic resonance spectroscopy

The solution conformation of the ribonuclease barnase has been determined by using 1H nuclear magnetic resonance (NMR) spectroscopy. The 20 structures were calculated by using 853 interproton distance restraints obtained from analyses of two-dimensional nuclear Overhauser spectra, 72 phi and 53 chi 1 torsion angle restraints, and 17 hydrogen-bond distance restraints. The calculated structures contain two alpha-helices (residues 6-18 and 26-34) and a five-stranded antiparallel beta-sheet (residues 50-55, 70-75, 85-91, 94-101, and 105-108). The core of the protein is formed by the packing of one of the alpha-helices (residues 6-18) onto the beta-sheet. The average RMS deviation between the calculated structures and the mean structure is 1.11 A for the backbone atoms and 1.75 A for all atoms. The protein is least well-defined in the N-terminal region and in three large loops. When these regions are excluded, the average RMS deviation between the calculated structures and the mean structure for residues 5-34, 50-56, 71-76, 85-109 is 0.62 A for the backbone atoms and 1.0 A for all atoms. The NMR-derived structure has been compared with the crystal structure of barnase [Mauguen et al. (1982) Nature (London) 297, 162-164].     

Refinement of the three-dimensional solution structure of barley serine proteinase inhibitor 2 and comparison with the structures in crystals.

The three-dimensional structure of barley serine proteinase inhibitor, CI-2, has been determined using nuclear magnetic resonance spectroscopy. The present structure determination is a refinement of the structure previously determined by us, using in the present case stereo-specific assignments, and a virtually complete set of assignments of the two-dimensional nuclear Overhauser spectrum. The structure determination is based on the identification of more than 1300 nuclear Overhauser effects, of which 961 were used in the structure calculation as distance restraints, and on 94 dihedral angle restraints, of which 31 are for chi 1 angles in defined chiral centers. These have been used to calculate a series of 20 three-dimensional structures using a combination of distance geometry, simulated annealing and restrained molecular dynamics. Each of the 20 structures was in agreement within less than 0.5 A of each of the distance restraints and with all dihedral angle restraints. When compared to the geometric average structure of the 20 refined structures the root-mean-square differences for the backbone atoms were 0.8 (+/- 0.2) A and for all atoms were 1.6 (+/- 0.2) A. By comparison, the values obtained for the structures determined previously were 1.4 (+/- 0.2) A and 2.1 (+/- 0.1) A, respectively. The structures were also compared to the structure determined in the crystalline state by X-ray diffraction showing root-mean-square differences of 1.6 (+/- 0.2) A and 2.8 (+/- 0.2) A for the backbone and all atoms, respectively. Common features of the solution structure and the two crystal structures are the four-stranded beta-structure, composed of a pair of parallel strands, and three pairs of antiparallel beta-strands flanked on one side by a 12-residue alpha-helix and on the other side by a loop containing the serine proteinase binding site. The new analysis of the structure has revealed an additional pair of antiparallel beta-strands, consisting of residues 65 to 67 and 81 to 83, that was not seen in either of the crystal structures or the previous solution structure. Identification of this was based on nuclear magnetic resonance evidence for the hydrogen bond (67HN to 81CO) not reported previously. Also the presence of a bifurcated hydrogen bond involving Phe69 CO and HN atoms of Ala77 and Gln78 was observed in solution but not in crystals. Minor differences between the two structures were observed in the phi-angles of residues Met59 and Glu60 in the inhibitory site.     

Determination of the three-dimensional solution structure of the antihypertensive and antiviral protein BDS-I from the sea anemone Anemonia sulcata: a study using nuclear magnetic resonance and hybrid distance geometry-dynamical simulated annealing

The three-dimensional solution structure of the antihypertensive and antiviral protein BDS-I from the sea anemone Anemonia sulcata has been determined on the basis of 489 interproton and 24 hydrogen-bonding distance restraints supplemented by 23 phi backbone and 21 chi 1 side-chain torsion angle restraints derived from nuclear magnetic resonance (NMR) measurements. A total of 42 structures is calculated by a hybrid metric matrix distance geometry-dynamical simulated annealing approach. Both the backbone and side-chain atom positions are well defined. The average atomic rms difference between the 42 individual SA structures and the mean structure obtained by averaging their coordinates is 0.67 +/- 0.12 A for the backbone atoms and 0.90 +/- 0.17 A for all atoms. The core of the protein is formed by a triple-stranded antiparallel beta-sheet composed of residues 14-16 (strand 1), 30-34 (strand 2), and 37-41 (strand 3) with an additional mini-antiparallel beta-sheet at the N-terminus (residues 6-9). The first and second strands of the triple-stranded antiparallel beta-sheet are connected by a long exposed loop (residues 17-30). A number of side-chain interactions are discussed in light of the structure.     

Determination of three-dimensional solution structure of waglerin I,a toxin from Trimeresurus wagleri,using 2D-NMR and molecular dynamics simulation

The solution conformation of a synthetic snake venom toxin waglerin I, has been determined by using proton nuclear magnetic resonance spectroscopy. By y a combination of various two-dimensional NMR techniques, the ¹H-NMR spectrum of waglerin I was completely assigned. A set of 247 interproton distance restraints was derived from nuclear Overhauser enhancement (NOE) measurements. These NOE constraints, in addition to the 2 dihedral angle restraints (from coupling constant measurements) and 7 ω torsion angle restraints for prolines, formed the basis of three-dimensional structure determined by molecular dynamics techniques. The 19 structures that were obtained satisfy the experimental restraints, and display small deviation from idealized covalent geometry. Analysis of converged structures indicates that the toxin has no special secondary structure. In the solution structure of waglerin I, the central ring region is well defined but the N- and C-termini possesses more disorder.     

High-resolution three-dimensional structure of reduced recombinant human thioredoxin in solution

The solution structure of recombinant human thioredoxin (105 residues) has been determined by nuclear magnetic resonance (NMR) spectroscopy combined with hybrid distance geometry-dynamical simulated annealing calculations. Approximate interproton distance restraints were derived from nuclear Overhauser effect (NOE) measurements. In addition, a large number of stereospecific assignments for beta-methylene protons and torsion angle restraints for phi, psi, and chi 1 were obtained by using a conformational grid search on the basis of the intraresidue and sequential NOE data in conjunction with 3JHN alpha and 3J alpha beta coupling constants. The structure calculations were based on 1983 approximate interproton distance restraints, 52 hydrogen-bonding restraints for 26 hydrogen bonds, and 98 phi, 71 psi, and 72 chi 1 torsion angle restraints. The 33 final simulated annealing structures obtained had an average atomic rms distribution of the individual structures about the mean coordinate positions of 0.40 +/- 0.06 A for the backbone atoms and 0.78 +/- 0.05 A for all atoms. The solution structure of human thioredoxin consists of a five-stranded beta-sheet surrounded by four alpha-helices, with an active site protrusion containing the two redox-active cysteines. The overall structure is similar to the crystal and NMR structures of oxidized [Katti, S. K., LeMaster, D. M., & Eklund, H. (1990) J. Mol. Biol. 212, 167-184] and reduced [Dyson, J. H., Gippert, G. P., Case, D. A., Holmgren, A., & Wright, P. (1990) Biochemistry 29, 4129-4136] Escherichia coli thioredoxin, respectively, despite the moderate 25% amino acid sequence homology. Several differences, however, can be noted. The human alpha 1 helix is a full turn longer than the corresponding helix in E. coli thioredoxin and is characterized by a more regular helical geometry. The helix labeled alpha 3 in human thioredoxin has its counterpart in the 3(10) helix of the E. coli protein and is also longer in the human protein. In contrast to these structural differences, the conformation of the active site loop in both proteins is very similar, reflecting the perfect sequence identity for a stretch of eight amino acid residues around the redox-active cysteines.     

Determination of the three-dimensional solution structure of the C-terminal domain of cellobiohydrolase I from Trichoderma reesei. A study using nuclear magnetic resonance and hybrid distance geometry-dynamical simulated annealing

The solution structure of a synthetic 36-residue polypeptide comprising the C-terminal cellulose binding domain of cellobiohydrolase I (CT-CBH I) from Trichoderma reesei was investigated by nuclear magnetic resonance (NMR) spectroscopy. The 1H NMR spectrum was completely assigned in a sequential manner by two-dimensional NMR techniques. A large number of stereospecific assignments for beta-methylene protons, as well as ranges for the phi, psi, and chi 1 torsion angles, were obtained on the basis of sequential and intraresidue nuclear Overhauser enhancement (NOE) and coupling constant data in combination with a conformational data base search. The structure calculations were carried out in an iterative manner by using the hybrid distance geometry-dynamical simulated annealing method. This involved computing a series of initial structures from a subset of the experimental data in order to resolve ambiguities in the assignments of some NOE cross-peaks arising from chemical shift degeneracy. Additionally, this permitted us to extend the stereospecific assignments to the alpha-methylene protons of glycine using information on phi torsion angles derived from the initial structure calculations. The final experimental data set consisted of 554 interproton distance restraints, 24 restraints for 12 hydrogen bonds, and 33 phi, 24 psi, and 25 chi 1 torsion angle restraints. CT-CBH I has two disulfide bridges whose pairing was previously unknown. Analysis of structures calculated with all three possible combinations of disulfide bonds, as well as without disulfide bonds, indicated that the correct disulfide bridge pairing was 8-25 and 19-35. Forty-one structures were computed with the 8-25 and 19-35 disulfide bridges, and the average atomic rms difference between the individual structures and the mean structure obtained by averaging their coordinates was 0.33 +/- 0.04 A for the backbone atoms and 0.52 +/- 0.06 A for all atoms. The protein has a wedgelike shape with an amphiphilic character, one face being predominantly hydrophilic and the other mainly hydrophobic. The principal element of secondary structure is made up of an irregular triple-stranded antiparallel beta-sheet composed of residues 5-9 (beta 1), 24-28 (beta 2), and 33-36 (beta 3) in which strand beta 3 is hydrogen bonded to the other two strands.(ABSTRACT TRUNCATED AT 400 WORDS)     

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.     

Three-dimensional structure of interleukin 8 in solution

The solution structure of the interleukin 8 (IL-8) dimer has been solved by nuclear magnetic resonance (NMR) spectroscopy and hybrid distance geometry-dynamical simulated annealing calculations. The structure determination is based on a total of 1880 experimental distance restraints (of which 82 are intersubunit) and 362 torsion angle restraints (comprising phi, psi, and chi 1 torsion angles). A total of 30 simulated annealing structures were calculated, and the atomic rms distribution about the mean coordinate positions (excluding residues 1-5 of each subunit) is 0.41 +/- 0.08 A for the backbone atoms and 0.90 +/- 0.08 A for all atoms. The three-dimensional solution structure of the IL-8 dimer reveals a structural motif in which two symmetry-related antiparallel alpha-helices, approximately 24 A long and separated by about 14 A, lie on top of a six-stranded antiparallel beta-sheet platform derived from two three-stranded Greek keys, one from each monomer unit. The general architecture is similar to that of the alpha 1/alpha 2 domains of the human class I histocompatibility antigen HLA-A2. It is suggested that the two alpha-helices form the binding site for the cellular receptor and that the specificity of IL-8, as well as that of a number of related proteins involved in cell-specific chemotaxis, mediation of cell growth, and the inflammatory response, is achieved by the distinct distribution of charged and polar residues at the surface of the helices.     

Solution structure of recombinant hirudin and the Lys-47----Glu mutant: a nuclear magnetic resonance and hybrid distance geometry-dynamical simulated annealing study

The solution structure of recombinant wild-type hirudin and of the putative active site mutant Lys-47----Glu has been investigated by nuclear magnetic resonance (NMR) spectroscopy at 600 MHz. The 1H NMR spectra of the two hirudin variants are assigned in a sequential manner with a combination of two-dimensional NMR techniques. Some assignments made in our previous paper [Sukumaran, D. K., Clore, G. M., Preuss, A., Zarbock, J., & Gronenborn, A. M. (1987) Biochemistry 26, 333-338] were found to be incorrect and are now corrected. Analysis of the NOE data indicates that hirudin consists of an N-terminal compact domain (residues 1-49) held together by three disulfide linkages and a disordered C-terminal tail (residues 50-65) which does not fold back on the rest of the protein. This last observation corrects conclusions drawn by us previously on hirudin extracted from its natural source, the leech Hirudo medicinalis. The improved sensitivity of the 600-MHz spectrometer relative to that of our old 500-MHz spectrometer, the availability of two variants with slightly different chemical shifts, and the additional information arising from stereospecific assignments of methylene beta-protons and methyl protons of valine have permitted the determination of the solution structure of hirudin with much greater precision than before. Structure calculations on the N-terminal domain using the hybrid distance geometry-dynamical simulated annealing method were based on 685 and 661 approximate interproton distance restraints derived from nuclear Overhauser enhancement (NOE) data for the wild-type and mutant hirudin, respectively, together with 16 distance restraints for 8 backbone hydrogen bonds identified on the basis of NOE and amide NH exchange data and 26 phi backbone and 18 chi 1 side-chain torsion angle restraints derived from NOE and three-bond coupling constant data. A total of 32 structures were computed for both the wild-type and mutant hirudin. The structure of residues 2-30 and 37-48 which form the core of the N-terminal domain is well determined in both cases with an average atomic rms difference between the individual structures and the respective mean structures of approximately 0.7 A for the backbone atoms and approximately 1 A for all atoms. As found previously, the orientation of the exposed finger of antiparallel beta-sheet (residues 31-36) with respect to the core could not be determined on the basis of the present data due to the absence of any long-range NOEs between the exposed finger and the core.(ABSTRACT TRUNCATED AT 250 WORDS)     

The solution structure of a B-DNA undecamer comprising a portion of the specific target site for the cAMP receptor protein in the gal operon. Refinement on the basis of interproton distance data.

A restrained least squares refinement of the solution structure of the double-stranded DNA undecamer 5'd(AAGTGT-GACAT).5'd(ATGTCACACTT) comprising a portion of the specific target site of the cAMP receptor protein in the gal operon is presented. The structure is refined on the basis of both distance and planarity restraints, 2331 in all. The distance restraints comprise 150 interproton distances determined from pre-steady state nuclear Overhauser enhancement measurements and 2159 other interatomic distances derived from idealized geometry (i.e., distances between covalently bonded atoms, between atoms defining fixed bond angles, and between atoms defining hydrogen bonding in AT and GC base pairs). Two refinements were carried out and in both cases the final RMS difference between the experimental and calculated interproton distances was 0.2 A. The difference between the two refined structures is small (overall RMS difference of 0.23 A) and represents the error in the refined coordinates. Although the refined structures have an overall B-type conformation there are large variations in many of the local conformational parameters including backbone and glycosidic bond torsion angles, helical twist and propellor twist, base roll and base tilt angles.     

Three-dimensional structure of the wild-type lac Pribnow promoter DNA in solution. Two-dimensional nuclear magnetic resonance studies and distance geometry calculations

The solution structure of a 12 base-pair DNA duplex containing the wt-lac promoter Pribnow sequence TATGTT has been studied by two-dimensional nuclear magnetic resonance spectroscopy. Proton assignments for the 24 sugar and base residues were obtained from two-dimensional correlated nuclear magnetic resonance and two-dimensional nuclear Overhauser effect spectra in both 2H2O and H2O, and by two-dimensional relayed coherence transfer nuclear magnetic resonance spectroscopy experiments. Time-dependent, two-dimensional nuclear Overhauser effect spectra were used to determine the initial cross-relaxation rates between 212 pairs of assigned protons, leading to 212 interproton distances in the double helix (8 to 9 per nucleotide). These distance constraints, and known bond lengths and angles, were entered into a distance matrix. After smoothing the bounds of the distance matrix, 12 trial matrices within the bounds constraints were independently generated and embedded in three-dimensional space using a distance geometry algorithm, to generate 12 trial structures. These trial structures were then refined until they no longer violated the distance matrix. The resulting structures are very similar at the local base-pair and nearest-neighbor base-pair level, but exhibit increasing variation at more distant and global levels. At the nearest-neighbor level, the A to T step and the G to T step within the Pribnow hexamer, as well as the G to T step preceding the hexamer, all exhibit very low screw pitch, i.e. 5(+/- 6) degrees. Conversely, the T to G step in the center of the promoter has a large screw pitch (47(+/- 2) degrees) and the T to G step at the 3' end of the promoter has a very large screw pitch (60(+/- 3) degrees). The limitations of nuclear magnetic resonance spectroscopy distance determination of structure are discussed in terms of resolution and spectral overlap of two-dimensional nuclear Overhauser effect crosspeaks. In the present duplex, the inability to measure several 1'-2' and 1'-2" distances resulted in underdetermination of the precise local sugar conformation for seven of the 24 residues, although the spatial position of all sugars was well defined.     

Solution structure of the module X2 1 of unknown function of the cellulosomal scaffolding protein CipC of Clostridium cellulolyticum

Multidimensional, homo- and heteronuclear magnetic resonance spectroscopy combined with dynamical annealing has been used to determine the structure of a 94 residue module (X2 1) of the scaffolding protein CipC from the anaerobic bacterium Clostridium cellulolyticum. An experimental data set comprising 1647 nuclear Overhauser effect-derived restraints, 105 hydrogen bond restraints and 66 phi torsion angle restraints was used to calculate 20 converging final solutions. The calculated structures have an average rmsd about the mean structure of 0.55(+/-0.11) A for backbone atoms and 1.40(+/-0.11) A for all heavy atoms when fitted over the secondary structural elements. The X2 1 module has an immunoglobulin-like fold with two beta-sheets packed against each other. One sheet contains three strands, the second contains four strands. An additional strand is intercalated between the beta-sandwich, as well as two turns of a 3(.10) helix. X2 1 has a surprising conformational stability and may act as a conformational linker and solubility enhancer within the scaffolding protein. The fold of X2 1 is very similar to that of telokin, titin Ig domain, hemolin D2 domain, twitchin immunoglobulin domain and the first four domains of the IgSF portion of transmembrane cell adhesion molecule. As a consequence, the X2 1 module is the first prokaryotic member assigned to the I set of the immunoglobulin superfamily even though no sequence similarity with any member of this superfamily could be detected.     

Determination of the complete three-dimensional structure of the trypsin inhibitor from squash seeds in aqueous solution by nuclear magnetic resonance and a combination of distance geometry and dynamical simulated annealing

The complete three-dimensional structure of the trypsin inhibitor from seeds of the squash Cucurbita maxima in aqueous solution was determined on the basis of 324 interproton distance constraints, 80 non-nuclear Overhauser effect distances, and 22 hydrogen-bonding constraints, supplemented by 27 phi backbone angle constraints derived from nuclear magnetic resonance measurements. The nuclear magnetic resonance input data were converted to the distance constraints in a semiquantitative manner after a sequence specific assignment of 1H spectra was obtained using two-dimensional nuclear magnetic resonance techniques. Stereospecific assignments were obtained for 17 of the 48 prochiral centers of the squash trypsin inhibitor using the floating chirality assignment introduced at the dynamical simulated annealing stage of the calculations. A total of 34 structures calculated by a hybrid distance geometry-dynamical simulated annealing method exhibit well-defined positions for both backbone and side-chain atoms. The average atomic root-mean-square difference between the individual structures and the minimized mean structure is 0.35(+/- 0.08) A for the backbone atoms and 0.89(+/- 0.17) A for all heavy atoms. The precision of the structure determination is discussed and correlated to the experimental input data.     

Determination of the solution structures of domains II and III of protein G from Streptococcus by 1H nuclear magnetic resonance.

We have used 1H nuclear magnetic resonance spectroscopy to determine the solution structures of two small (61 and 64 residue) immunoglobulin G (IgG)-binding domains from protein G, a cell-surface protein from Streptococcus strain G148. The two domains differ in sequence by four amino acid substitutions, and differ in their affinity for some subclasses of IgG. The structure of domain II was determined using a total of 478 distance restraints, 31 phi and 9 chi 1 dihedral angle restraints; that of domain III was determined using a total of 445 distance restraints, 31 phi and 9 chi 1 dihedral angle restraints. A protocol which involved distance geometry, simulated annealing and restrained molecular dynamics was used to determine ensembles of 40 structures consistent with these restraints. The structures are found to consist of an alpha-helix packed against a four-stranded antiparallel-parallel-antiparallel beta-sheet. The structures of the two domains are compared to each other and to the reported structure of a similar domain from a protein G from a different strain of Streptococcus. We conclude that the difference in affinity of domains II and III for IgG is due to local changes in amino acid side-chains, rather than a more extensive change in conformation, suggesting that one or more of the residues which differ between them are directly involved in interaction with IgG.     

The three-dimensional structure of alpha1-purothionin in solution: combined use of nuclear magnetic resonance, distance geometry and restrained molecular dynamics

The determination of the three-dimensional solution structure of α1-purothionin using a combination of metric matrix distance geometry and restrained molecular dynamics calculations based on n.m.r. data is presented. The experimental data comprise complete sequence-specific proton resonance assignments, a set of 310 approximate interproton distance restraints derived from nuclear Overhauser effects, 27 Ø backbone torsion angle restraints derived from vicinal coupling constants, 4 distance restraints from hydrogen bonds and 12 distance restraints from disulphide bridges. The average atomic rms difference between the final nine converged structures and the mean structure obtained by averaging their coordinates is 1.5 ± 0.1 å for the backbone atoms and 2.0 ± 0.1 å for all atoms. The overall shape of α1-purothionin is that of the capital letter L, similar to that of crambin, with the longer arm comprising two approximately parallel α-helices and the shorter arm a strand and a mini anti-parallel β sheet.     

Solution structure of a lipid transfer protein extracted from rice seeds. Comparison with homologous proteins.

Nuclear magnetic resonance (NMR) spectroscopy was used to determine the three dimensional structure of rice nonspecific lipid transfer protein (ns-LTP), a 91 amino acid residue protein belonging to the broad family of plant ns-LTP. Sequence specific assignment was obtained for all but three HN backbone 1H resonances and for more than 95% of the 1H side-chain resonances using a combination of 1H 2D NOESY; TOCSY and COSY experiments at 293 K. The structure was calculated on the basis of four disulfide bridge restraints, 1259 distance constraints derived from 1H-1H Overhauser effects, 72 phi angle restraints and 32 hydrogen-bond restraints. The final solution structure involves four helices (H1: Cys3-Arg18, H2: Ala25-Ala37, H3: Thr41-Ala54 and H4: Ala66-Cys73) followed by a long C-terminal tail (T) with no observable regular structure. N-capping residues (Thr2, Ser24, Thr40), whose side-chain oxygen atoms are involved in hydrogen bonds with i + 3 amide proton additionally stabilize the N termini of the first three helices. The fourth helix involving Pro residues display a mixture of alpha and 3(10) conformation. The rms deviation of 14 final structures with respect to the average structure is 1.14 +/- 0.16 A for all heavy atoms (C, N, O and S) and 0.72 +/- 0.01 A for the backbone atoms. The global fold of rice ns-LTP is close to the previously published structures of wheat, barley and maize ns-LTPs exhibiting nearly identical pattern of the numerous sequence specific interactions. As reported previously for different four-helix topology proteins, hydrophobic, hydrogen bonding and electrostatic mechanisms of fold stabilization were found for the rice ns-LTP. The sequential alignment of 36 ns-LTP primary structures strongly suggests that there is a uniform pattern of specific long-range interactions (in terms of sequence), which stabilize the fold of all plant ns-LTPs.     

Solution structure of neurotoxin I from the sea anemone Stichodactyla helianthus. A nuclear magnetic resonance, distance geometry, and restrained molecular dynamics study

The three-dimensional structure of the sea anemone polypeptide Stichodactyla helianthus neurotoxin I in aqueous solution has been determined using distance geometry and restrained molecular dynamics simulations based on NMR data acquired at 500 MHz. A set of 470 nuclear Overhauser enhancement values was measured, of which 216 were used as distance restraints in the structure determination along with 15 dihedral angles derived from coupling constants. After restrained molecular dynamics refinement, the eight structures that best fit the input data form a closely related family. They describe a structure that consists of a core of twisted, four-stranded, antiparallel beta-sheet encompassing residues 1-3, 19-24, 29-34, and 40-47, joined by three loops, two of which are well defined by the NMR data. The third loop, encompassing residues 7-16, is poorly defined by the data and is assumed to undergo conformational averaging in solution. Pairwise root mean square displacement values for the backbone heavy atoms of the eight best structures are 1.3 +/- 0.2A when the poorly defined loop is excluded and 3.6 +/- 1.0A for all backbone atoms. Refinement using restrained molecular dynamics improved the quality of the structures generated by distance geometry calculations with respect to the number of nuclear Overhauser enhancements violated, the size of the total distance violations and the total potential energies of the structures. The family of structures for S. heliathus neurotoxin I is compared with structures of related sea anemone proteins that also bind to the voltage-gated sodium channel.     

The solution conformation of the antibacterial peptide cecropin A: a nuclear magnetic resonance and dynamical simulated annealing study

The solution conformation of the antibacterial polypeptide cecropin A from the Cecropia moth is investigated by nuclear magnetic resonance (NMR) spectroscopy under conditions where it adopts a fully ordered structure, as judged by previous circular dichroism studies [Steiner, H. (1982) FEBS Lett. 137, 283-287], namely, 15% (v/v) hexafluoroisopropyl alcohol. By use of a combination of two-dimensional NMR techniques the 1H NMR spectrum of cecropin A is completely assigned. A set of 243 approximate interproton distance restraints is derived from nuclear Overhauser enhancement (NOE) measurements. These, together with 32 distance restraints for the 16 intrahelical hydrogen bonds identified on the basis of the pattern of short-range NOEs, form the basis of a three-dimensional structure determination by dynamical simulated annealing [Nilges, M., Clore, G.M., & Gronenborn, A.M. (1988) FEBS Lett. 229, 317-324]. The calculations are carried out starting from three initial structures, an alpha-helix, an extended beta-strand, and a mixed alpha/beta structure. Seven independent structures are computed from each starting structure by using different random number seeds for the assignments of the initial velocities. All 21 calculated structures satisfy the experimental restraints, display very small deviations from idealized covalent geometry, and possess good nonbonded contacts. Analysis of the 21 converged structure indicates that there are two helical regions extending from residues 5 to 21 and from residues 24 to 37 which are very well defined in terms of both atomic root mean square differences and backbone torsion angles. For the two helical regions individually the average backbone rms difference between all pairs of structures is approximately 1 A. The long axes of the two helices lie in two planes, which are at an angle of 70-100 degrees to each other. The orientation of the helices within these planes, however, cannot be determined due to the paucity of NOEs between the two helices.     

Total assignments, including four aromatic residues, and sequence confirmation of the decapeptide tyrocidine A using difference double resonance. Qualitative nuclear overhauser effect criteria for beta turn and antiparallel beta-pleated sheet conformations.

The complete assignments of all the proton magnetic resonance signals from each NH-CalphaH-CbetaH2 moiety in a complex peptide containing several residues of the same type has not yet been achieved without specific or stereospecific isotopic enrichment. We report the sequencing and proton magnetic resonance spectral assignments, including those of 4 aromatic residues, of tyrocidine A, an analog of the decapeptide gramicidin S. Two complementary methods, proton-proton nuclear Overhauser enhancements and scalar decoupling, evaluated by two distinct forms of difference double resonance, were used. All chemical shifts, scalar coupling constants, and [1H:1H] nuclear Overhauser enhancements for the backbone protons are reported. The [1H:1H] nuclear Overhauser enhancements are consistent with tyrocidine A possessing a beta-I turn/beta-II' turn/antiparallel beta-pleated sheet conformation. In addition to the previously proposed nuclear Overhauser enhancement criteria for beta turns and antiparallel beta sheets, another criterion for identifying the antiparallel beta sheet is demonstrated; namely, the nuclear Overhauser enhancement between 2 CalphaH protons of the central resisdues, in this case the Phe7CalphaH and Orn2CalphaH.     

Three-dimensional solution structure of the E3-binding domain of the dihydrolipoamide succinyltransferase core from the 2-oxoglutarate dehydrogenase multienzyme complex of Escherichia coli.

The three-dimensional solution structure of a 51-residue synthetic peptide comprising the dihydrolipoamide dehydrogenase (E3)-binding domain of the dihydrolipoamide succinyltransferase (E2) core of the 2-oxoglutarate dehydrogenase multienzyme complex of Escherichia coli has been determined by nuclear magnetic resonance spectroscopy and hybrid distance geometry-dynamical simulated annealing calculations. The structure is based on 630 approximate interproton distance and 101 torsion angle (phi, psi, chi 1) restraints. A total of 56 simulated annealing structures were calculated, and the atomic rms distribution about the mean coordinate positions for residues 12-48 of the synthetic peptide is 1.24 A for the backbone atoms, 1.68 A for all atoms, and 1.33 A for all atoms excluding the six side chains which are disordered at chi 1 and the seven which are disordered at chi 2; when the irregular partially disordered loop from residues 31 to 39 is excluded, the rms distribution drops to 0.77 A for the backbone atoms, 1.55 A for all atoms, and 0.89 A for ordered side chains. Although proton resonance assignments for the N-terminal 11 residues and the C-terminal 3 residues were obtained, these two segments of the polypeptide are disordered in solution as evidenced by the absence of nonsequential nuclear Overhauser effects. The solution structure of the E3-binding domain consists of two parallel helices (residues 14-23 and 40-48), a short extended strand (24-26), a five-residue helical-like turn, and an irregular (and more disordered) loop (residues 31-39). This report presents the first structure of an E3-binding domain from a 2-oxo acid dehydrogenase complex.(ABSTRACT TRUNCATED AT 250 WORDS)