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 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)     

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.     

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 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.     

Three-dimensional structure in solution of barwin, a protein from barley seed.

The solution structure of a 125-residue basic protein, barwin, has been determined using 1H nuclear magnetic resonance spectroscopy. This protein is closely related to domains in proteins encoded by wound-induced genes in plants. Analysis of the 1H nuclear Overhauser spectrum revealed the assignment of more than 1400 nuclear Overhauser effects. Twenty structures were calculated based on 676 nontrivial distance restraints, 152 torsion angle restraints (92 phi, 56 chi 1, and 4 omega for proline), and stereospecific assignments of 38 chiral centers, using distance geometry, simulated annealing, and restrained energy minimization. None of the distance restraints was violated by more than 0.5 A in any of the 20 structures, and none of the torsion angle restraints was violated by more than 1 degree in any of the structures. The RMS difference between the calculated and target interproton distance restraints is 0.033 A, and the average atomic RMS differences between the 20 structures and their geometric average are 1.23 A for backbone atoms and 1.73 A for all heavy atoms. The dominating structural feature of the protein is a well-defined four-stranded antiparallel beta-sheet, two parallel beta-sheets packed antiparallel to each other and four short alpha-helices. The binding site of barwin to the tetramer N-acetylglucosamine has been qualitatively investigated, and the dissociation constant of the complex has been determined using one-dimensional 1H nuclear magnetic resonance spectroscopy.     

The determination of the three-dimensional structure of barley serine proteinase inhibitor 2 by nuclear magnetic resonance, distance geometry and restrained molecular dynamics

The solution structure of the 64 residue structured domain (residues 20-83) of barley serine proteinase inhibitor 2 (BSPI-2) is determined on the basis of 403 interproton distance, 34 phi backbone torsion angle and 26 hydrogen bonding restraints derived from n.m.r. measurements. A total of 11 converged structures were computed using a metric matrix distance geometry algorithm and refined by restrained molecular dynamics. The average rms difference between the final 11 structures and the mean structure obtained by averaging their coordinates is 1.4 +/- 0.2 A for the backbone atoms and 2.1 +/- 0.1 A for all atoms. The overall structure, which is almost identical to that found by X-ray crystallography, is disc shaped and consists of a central four component mixed parallel and antiparallel beta-sheet flanked by a 13 residue alpha-helix on one side and the reactive site loop on the other.     

Application of molecular dynamics with interproton distance restraints to three-dimensional protein structure determination. A model study of crambin

The applicability of restrained molecular dynamics for the determination of three-dimensional protein structures on the basis of short interproton distances (less than 4 A) that can be realistically determined from nuclear magnetic resonance measurements in solution is assessed. The model system used is the 1.2 A resolution crystal structure of the 46 residue protein crambin, from which a set of 240 approximate distance restraints, divided into three ranges (2.5 +/- 0.5, 3.0+0.5(-1.0) and 4 +/- 1 A), is derived. This interproton distance set comprises 159 short-range ([i-j] less than or equal to 5) and 56 ([i-j] greater than 5) long-range inter-residue distances and 25 intra-residue distances. Restrained molecular dynamics are carried out using a number of different protocols starting from two initial structures: a completely extended beta-strand; and an extended structure with two alpha-helices in the same positions as in the crystal structure (residues 7 to 19, and 23 to 30) and all other residues in the form of extended beta-strands. The root-mean-square (r.m.s.) atomic differences between these two initial structures and the crystal structure are 43 A and 23 A, respectively. It is shown that, provided protocols are used that permit the secondary structure elements to form at least partially prior to folding into a tertiary structure, convergence to the correct final structure, both globally and locally, is achieved. The r.m.s. atomic differences between the converged restrained dynamics structures and the crystal structure range from 1.5 to 2.2 A for the backbone atoms and from 2.0 to 2.8 A for all atoms. The r.m.s. atomic difference between the X-ray structure and the structure obtained by first averaging the co-ordinates of the converged restrained dynamics structures is even smaller: 1.0 A for the backbone atoms and 1.6 A for all atoms. These results provide a measure with which to judge future experimental results on proteins whose crystal structures are unknown. In addition, from an examination of the dynamics trajectories, it is shown that the convergence pathways followed by the various simulations are different.     

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].     

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.     

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.     

Three-dimensional solution structure of the B domain of staphylococcal protein A: comparisons of the solution and crystal structures.

The three-dimensional solution structure of the recombinant B domain (FB) of staphylococcal protein A, which specifically binds to the Fc portion of immunoglobulin G, was determined by NMR spectroscopy and hybrid distance geometry-dynamical simulated annealing calculations. On the basis of 692 experimental constraints including 587 distance constraints obtained from the nuclear Overhauser effect (NOE), 57 torsion angle (phi, chi 1) constraints, and 48 constraints associated with 24 hydrogen bonds, a total of 10 converged structures of FB were obtained. The atomic root mean square difference among the 10 converged structures is 0.52 +/- 0.10 A for the backbone atoms and 0.98 +/- 0.08 A for all heavy atoms (excluding the N-terminal segment from Thr1 to Glu9 and the C-terminal segment from Gln56 to Ala60, which are partially disordered). FB is composed of a bundle of three alpha-helices, i.e., helix I (Gln10-His19), helix II (Glu25-Asp37), and helix III (Ser42-Ala55). Helix II and helix III are antiparallel to each other, whereas the long axis of helix I is tilted at an angle of about 30 degrees with respect to those of helix II and helix III. Most of the hydrophobic residues of FB are buried in the interior of the bundle of the three helices. It is suggested that the buried hydrophobic residues form a hydrophobic core, contributing to the stability of FB.(ABSTRACT TRUNCATED AT 250 WORDS)     

The three-dimensional structure of guanine-specific ribonuclease F1 in solution determined by NMR spectroscopy and distance geometry.

Two-dimensional 1H-NMR studies have been performed on ribonuclease F1 (RNase F1), which contains 106 amino acid residues. Sequence-specific resonance assignments were accomplished for the backbone protons of 99 amino acid residues and for most of their side-chain protons. The three-dimensional structures were constructed on the basis of 820 interproton-distance restraints derived from NOE, 64 distance restraints for 32 hydrogen bonds and 33 phi torsion-angle restraints. A total of 40 structures were obtained by distance geometry and simulated-annealing calculations. The average root-mean-square deviation (residues 1-106) between the 40 converged structures and the mean structure obtained by averaging their coordinates was 0.116 +/- 0.018 nm for the backbone atoms and 0.182 +/- 0.015 nm for all atoms including the hydrogen atoms. RNase F1 was determined to be an alpha/beta-type protein. A well-defined structure constitutes the core region, which consists of a small N-terminal beta-sheet (beta 1, beta 2) and a central five-stranded beta-sheet (beta 3-beta 7) packed on a long helix. The structure of RNase F1 has been compared with that of RNase T1, which was determined by X-ray crystallography. Both belong to the same family of microbial ribonucleases. The polypeptide backbone fold of RNase F1 is basically identical to that of RNase T1. The conformation-dependent chemical shifts of the C alpha protons are well conserved between RNase F1 and RNase T1. The residues implicated in catalysis are all located on the central beta-sheet in a geometry similar to that of RNase T1.     

Solution structure of the PDZ2 domain from human phosphatase hPTP1E and its interactions with C-terminal peptides from the Fas receptor

The solution structure of the second PDZ domain (PDZ2) from human phosphatase hPTP1E has been determined using 2D and 3D heteronuclear NMR experiments. The binding of peptides derived from the C-terminus of the Fas receptor to PDZ2 was studied via changes in backbone peptide and protein resonances. The structure is based on a total of 1387 nonredundant experimental NMR restraints including 1261 interproton distance restraints, 45 backbone hydrogen bonds, and 81 torsion angle restraints. Analysis of 30 lowest-energy structures resulted in rmsd values of 0.41 +/- 0.09 A for backbone atoms (N, Calpha, C') and 1.08 +/- 0.10 A for all heavy atoms, excluding the disordered N- and C-termini. The hPTP1E PDZ2 structure is similar to known PDZ domain structures but contains two unique structural features. In the peptide binding domain, the first glycine of the GLGF motif is replaced by a serine. This serine appears to replace a bound water observed in PDZ crystal structures that hydrogen bonds to the bound peptide's C-terminus. The hPTP1E PDZ2 structure also contains an unusually large loop following strand beta2 and proximal to the peptide binding site. This well-ordered loop folds back against the PDZ domain and contains several residues that undergo large amide chemical shift changes upon peptide binding. Direct observation of peptide resonances demonstrates that as many as six Fas peptide residues interact with the PDZ2 domain.     

Determination of the spatial structure of insectotoxin 15A from Buthus erpeus by (1)H-NMR spectroscopy data]

The solution structure of insectotoxin 15A (35 residues) from scorpion Buthus eupeus was determined on the basis of 386 interproton distance restraints 12 hydrogen-bonding restraints and 113 dihedral angle restraints derived from 1H NMR experiments. A group of 20 structures was calculated with the distance geometry program DIANA followed by the restrained energy minimization with the program CHARMM. The atomic RMS distribution about the mean coordinate position is 0.64 +/- 0.11 A for the backbone atoms and 1.35 +/- 0.20 A for all atoms. The structure contains an alpha-helix (residues 10-20) and a three-stranded antiparallel beta-sheet (residues 2-5, 24-28 and 29-33). A pairing of the eight cysteine residues of insectotoxin 15A was established basing on NMR data. Three disulfide bridges (residues 2-19, 16-31 and 20-33) connect the alpha-helix with the beta-sheet, and the fourth one (5-26) joins beta-strands together. The spatial fold of secondary structure elements (the alpha-helix and the beta-sheet) of the insectotoxin 15A is very similar to those of the other short and long scorpion toxins in spite of a low (about 20%) sequence homology.     

Solution structure of a polypeptide dimer comprising the fourth Ca(2+)-binding site of troponin C by nuclear magnetic resonance spectroscopy

The structure of a 39 amino acid proteolytic fragment of rabbit skeletal troponin C containing the fourth Ca(2+)-binding site has been determined by an approach involving nuclear magnetic resonance (NMR) spectroscopy combined with hybrid distance geometry-dynamical simulated annealing calculations. Hydrodynamic and NMR evidence establishes unambiguously that the fragment forms a stable dimer in solution in the presence of excess Ca2+. The calculation of the dimeric structure is based on a total of 1056 experimental restraints comprising 422 interproton distances, 35 phi, 28 psi, and 28 chi 1 torsion angle restraints within each subunit, 30 intermonomer distance restraints, and 6 Ca2+ restraints per subunit. A total of 48 final structures were calculated having an rms deviation about the mean atomic backbone coordinate positions of 1.0 A for residues Asp128-Glu156. The solution structure consists of a dimer of helix-loop-helix motifs related by a 2-fold axis of symmetry. The overall architecture of the dimer is very similar to the C-terminal domain in the crystal structure of chicken skeletal troponin C.     

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)     

Three-dimensional structure of potato carboxypeptidase inhibitor in solution. A study using nuclear magnetic resonance, distance geometry, and restrained molecular dynamics

The solution conformation of potato carboxypeptidase inhibitor (CPI) has been investigated by 1H NMR spectroscopy. The spectrum is assigned in a sequential manner by using two-dimensional NMR techniques to identify through-bond and through-space (less than 5 A) connectivities. A set of 309 approximate interproton distance restraints is derived from the two-dimensional nuclear Overhauser enhancement spectra and used as the basis of a three-dimensional structure determination by a combination of metric matrix distance geometry and restrained molecular dynamics calculations. A total of 11 converged distance geometry structures were computed and refined by using restrained molecular dynamics. The average atomic root mean square (rms) difference between the final 11 structures and the mean structure obtained by averaging their coordinates is 1.4 +/- 0.3 A for residues 2-39 and 0.9 +/- 0.2 A for residues 5-37. The corresponding values for all atoms are 1.9 +/- 0.3 and 1.4 +/- 0.2 A, respectively. The larger values for residues 2-38 relative to those for residues 5-37 arise from the fact that the positions of the N- (residues 1-4) and C- (residues 38-39) terminal tails are rather poorly determined, whereas those of the core of the protein (residues 5-37) are well determined by the experimental interproton distance data. The computed structures are very close to the X-ray structure of CPI in its complex with carboxypeptidase, and the backbone atomic rms difference between the mean of the computed structures and the X-ray structure is only 1.2 A. Nevertheless, there are some real differences present which are evidenced by significant deviations between the experimental upper interproton distance limits and the corresponding interproton distances derived from the X-ray structure. These principally occur in two regions, residues 18-20 and residues 28-30, the latter comprising part of the region of secondary contacts between CPI and carboxypeptidase in the X-ray structure.     

Three-dimensional solution structure of the sodium channel agonist/antagonist delta-conotoxin TxVIA

The three-dimensional solution structure of delta-conotoxin TxVIA, a 27-mer peptide agonist/antagonist of sodium channels, was determined by two-dimensional (1)H NMR spectroscopy with simulated annealing calculations. A total of 20 converged structures of delta-conotoxin TxVIA were obtained on the basis of 360 distance constraints obtained from nuclear Overhauser effect connectivities, 28 torsion angle constraints, and 27 constraints associated with hydrogen bonds and disulfide bonds. The atomic root mean square difference about the averaged coordinate positions is 0.35 +/- 0.07 A for the backbone atoms (N, C(alpha), C) and 0.98 +/- 0.14 A for all heavy atoms of the entire peptide. The molecular structure of delta-conotoxin TxVIA is composed of a short triple-stranded antiparallel beta-sheet. The overall beta-sheet topology is +2x, -1, which is the same as those for other conotoxins. However, the three-dimensional structure of delta-conotoxin TxVIA has an unusual hydrophobic patch on one side of the molecule, which may play an important role in the sodium channel binding. These results provide a molecular basis for understanding the mechanism of sodium channel modulation through the toxin-channel interaction and insight into the discrimination of different ion channels.     

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.