The solution structure of eglin c based on measurements of many NOEs and coupling constants and its comparison with X‐ray structures

A high‐precision solution structure of the elastase inhibitor eglin c was determined by NMR and distance geometry calculations. A large set of 947 nuclear Overhauser (NOE) distance constraints was identified, 417 of which were quantified from two‐dimensional NOE spectra at short mixing times. In addition, a large number of homonuclear 1H‐1H and heteronuclear 1H‐15N vicinal coupling constants were used, and constraints on 42 χ1 and 38 ϕ angles were obtained. Structure calculations were carried out using the distance geometry program DG‐II. These calculations had a high convergence rate, in that 66 out of 75 calculations converged with maximum residual NOE violations ranging from 0.17 Å to 0.47 Å. The spread of the structures was characterized with average root mean square deviations () between the structures and a mean structure. To calculate the unbiased toward any single structure, a new procedure was used for structure alignment. A canonical structure was calculated from the mean distances, and all structures were aligned relative to that. Furthermore, an angular order parameter S was defined and used to characterize the spread of structures in torsion angle space. To obtain an accurate estimate of the precision of the structure, the number of calculations was increased until the and the angular order parameters stabilized. This was achieved after approximately 40 calculations. The structure consists of a well‐defined core whose backbone deviates from the canonical structure ca. 0.4 Å, a disordered N‐terminal heptapeptide whose backbone deviates by 0.8–12 Å, and a proteinase‐binding loop whose backbone deviates up to 3.0 Å. Analysis of the angular order parameters and inspection of the structures indicates that a hinge‐bending motion of the binding loop may occur in solution. Secondary structures were analyzed by comparison of dihedral angle patterns. The high precision of the structure allows one to identify subtle differences with four crystal structures of eglin c determined in complexes with proteinases.

[1]  M G Rossmann,et al.  Comparison of super-secondary structures in proteins. , 1973, Journal of molecular biology.

[2]  K Wüthrich,et al.  Determination of the complete three-dimensional structure of the alpha-amylase inhibitor tendamistat in aqueous solution by nuclear magnetic resonance and distance geometry. , 1988, Journal of molecular biology.

[3]  C. Betzel,et al.  Crystal structure of a complex between thermitase from Thermoactinomyces vulgaris and the leech inhibitor eglin , 1988, FEBS letters.

[4]  Richard R. Ernst,et al.  Coherence transfer by isotropic mixing: Application to proton correlation spectroscopy , 1983 .

[5]  G. Montelione,et al.  Accurate measurements of long-range heteronuclear coupling constants from homonuclear 2D NMR spectra of isotope-enriched proteins , 1989 .

[6]  Ad Bax,et al.  MLEV-17-based two-dimensional homonuclear magnetization transfer spectroscopy , 1985 .

[7]  M. James,et al.  Crystal and molecular structure of the inhibitor eglin from leeches in complex with subtilisin Carlsberg , 1985, FEBS letters.

[8]  Dieter Suter,et al.  Two-dimensional chemical exchange and cross-relaxation spectroscopy of coupled nuclear spins , 1981 .

[9]  K. Wüthrich NMR of proteins and nucleic acids , 1988 .

[10]  S. Hyberts,et al.  Sequence-specific 1H NMR assignments and secondary structure of eglin c. , 1990, Biochemistry.

[11]  K. Wilson,et al.  Refined crystal structures of subtilisin novo in complex with wild-type and two mutant eglins. Comparison with other serine proteinase inhibitor complexes. , 1991, Journal of molecular biology.

[12]  K. Wüthrich,et al.  Protein conformation and proton nuclear-magnetic-resonance chemical shifts. , 1983, European journal of biochemistry.

[13]  A. Pardi,et al.  Hydrogen bond length and proton NMR chemical shifts in proteins , 1983 .

[14]  Jeffrey W. Peng,et al.  2D heteronuclear NMR measurements of spin-lattice relaxation times in the rotating frame of X nuclei in heteronuclear HX spin systems , 1991 .

[15]  W. Bode,et al.  Refined 1.2 A crystal structure of the complex formed between subtilisin Carlsberg and the inhibitor eglin c. Molecular structure of eglin and its detailed interaction with subtilisin. , 1986, The EMBO journal.

[16]  K. Wüthrich,et al.  A systematic approach to the suppression of J cross peaks in 2D exchange and 2D NOE spectroscopy , 1985 .

[17]  V. Bystrov Spin—spin coupling and the conformational states of peptide systems , 1976 .

[18]  K Wüthrich,et al.  A two-dimensional nuclear Overhauser enhancement (2D NOE) experiment for the elucidation of complete proton-proton cross-relaxation networks in biological macromolecules. , 1980, Biochemical and biophysical research communications.

[19]  M. Eulitz,et al.  Structure of the elastase-cathepsin G inhibitor of the leech Hirudo medicinalis. , 1980, Hoppe-Seyler's Zeitschrift fur physiologische Chemie.

[20]  Timothy F. Havel,et al.  Protein structures in solution by nuclear magnetic resonance and distance geometry. The polypeptide fold of the basic pancreatic trypsin inhibitor determined using two different algorithms, DISGEO and DISMAN. , 1987, Journal of molecular biology.

[21]  A. Gronenborn,et al.  Comparison of the solution and X-ray structures of barley serine proteinase inhibitor 2. , 1987, Protein engineering.

[22]  Timothy F. Havel,et al.  The sampling properties of some distance geometry algorithms applied to unconstrained polypeptide chains: A study of 1830 independently computed conformations , 1990, Biopolymers.

[23]  M. James,et al.  Structural comparison of two serine proteinase-protein inhibitor complexes: eglin-c-subtilisin Carlsberg and CI-2-subtilisin Novo. , 1988, Biochemistry.

[24]  Gordon M. Crippen,et al.  Stable calculation of coordinates from distance information , 1978 .

[25]  A. J. Shaka,et al.  Iterative schemes for bilinear operators; application to spin decoupling , 1988 .

[26]  G. Wider,et al.  A heteronuclear three-dimensional NMR experiment for measurements of small heteronuclear coupling constants in biological macromolecules , 1989 .

[27]  Richard R. Ernst,et al.  Coherence transfer in the rotating frame , 1979 .

[28]  F M Poulsen,et al.  The determination of the three-dimensional structure of barley serine proteinase inhibitor 2 by nuclear magnetic resonance, distance geometry and restrained molecular dynamics. , 1987, Protein engineering.

[29]  J. Richardson,et al.  The anatomy and taxonomy of protein structure. , 1981, Advances in protein chemistry.

[30]  M. James,et al.  Crystal and molecular structure of the serine proteinase inhibitor CI-2 from barley seeds. , 1988, Biochemistry.

[31]  S. Hyberts,et al.  Stereospecific assignments of side-chain protons and characterization of torsion angles in Eglin c. , 1987, European journal of biochemistry.

[32]  Timothy F. Havel An evaluation of computational strategies for use in the determination of protein structure from distance constraints obtained by nuclear magnetic resonance. , 1991, Progress in biophysics and molecular biology.

[33]  Djordje Musil,et al.  The high-resolution X-ray crystal structure of the complex formed between subtilisin Carlsberg and eglin c, an elastase inhibitor from the leech Hirudo medicinalis Structural analysis, subtilisin structure and interface geometry , 1987 .

[34]  Richard R. Ernst,et al.  Investigation of exchange processes by two‐dimensional NMR spectroscopy , 1979 .

[35]  C. Betzel,et al.  Molecular dynamics refinement of a thermitase-eglin-c complex at 1.98 A resolution and comparison of two crystal forms that differ in calcium content. , 1989, Journal of molecular biology.

[36]  K Wüthrich,et al.  Sequential resonance assignments in protein 1H nuclear magnetic resonance spectra. Computation of sterically allowed proton-proton distances and statistical analysis of proton-proton distances in single crystal protein conformations. , 1982, Journal of molecular biology.