The structure of the complex formed by bovine trypsin and bovine pancreatic trypsin inhibitor

The structure of the complex between anhydro-trypsin and pancreatic trypsin inhibitor has been determined by difference Fourier techniques using phases obtained from the native complex (Huber et al., 1974). It was refined independently by constrained crystallographic refinement at 1.9 å resolution. The anhydro-complex has Ser 195 converted to dehydro-alanine. There were no other significant structural changes. In particular, the high degree of pyramidalization of the C atom of Lys 15 (I) of the inhibitor component observed in the native complex is maintained in the anhydro-species.     

The compact state of reduced bovine pancreatic trypsin inhibitor is not the compact molten globule.

Reduced bovine pancreatic trypsin inhibitor (BPTI) has been shown to be in a compact state [(1988) Biochemistry 27, 8889-8893]. This leads to the proposal that this compact state may be a compact molten globule folding intermediate. Optical rotatory dispersion in the visible region failed to show the presence of pronounced secondary structures in the reduced BPTI and no binding of 8-anilino-1-naphthalenesulphonic acid to reduced BPTI could be detected. Yet, no cooperative thermal transition was detected by tyrosine fluorescence. These experiments show that reduced BPTI is not in the compact molten globule state.     

Flexibility of bovine pancreatic trypsin inhibitor

The native conformation of a protein may be expressed in terms of the dihedral angles, phi's and psi's for the backbone, and kappa's for the side chains, for a given geometry (bond lengths and bond angles). We have developed a method to obtain the dihedral angles for a low-energy structure of a protein, starting with the X-ray structure; it is applied here to examine the degree of flexibility of bovine pancreatic trypsin inhibitor. Minimization of the total energy of the inhibitor (including nonbonded, electrostatic, torsional, hydrogen bonding, and disulfide loop energies) yields a conformation having a total energy of -221 kcal/mol and a root mean square deviation between all atoms of the computed and experimental structures of 0.63 A. The optimal conformation is not unique, however, there being at least two other conformations of low-energy (-222 and -220 kcal/mol), which resemble the experimental one (root mean square deviations of 0.66 and 0.64 A, respectively). These three conformations are located in different positions in phi, psi space, i.e., with a total deviation of 81 degrees, 100 degrees and 55 degrees from each other (with a root mean square deviation of several degrees per dihedral angle from each other). The nonbonded energies of the backbones, calculated along lines in phi, psi space connecting these three conformations, are all negative, without any intervening energy barriers (on an energy contour map in the phi, psi plane). Side chains were attached at several representative positions in this plane, and the total energy was minimized by varying the kappa's. The energies were of approximately the same magnitude as the previous ones, indicating that the conformation of low energy is flexible to some extent in a restricted region of phi, psi space. Interestingly, the difference delta phi i+1 in phi i+1 for the (i + 1)th residue from one conformation to another is approximately the same as -delta psi i for the ith residue; i.e., the plane of the peptide group between the ith and (i + 1)th residues re-orient without significant changes in the positions of the other atoms. The flexibility of the orientations of the planes of the peptide groups is probably coupled in a cooperative manner to the flexibility of the positions of the backbone and side-chain atoms.     

Hydrogen exchange kinetics of bovine pancreatic trypsin inhibitor beta-sheet protons in trypsin-bovine pancreatic trypsin inhibitor, trypsinogen-bovine pancreatic trypsin inhibitor, and trypsinogen-isoleucylvaline-bovine pancreatic trypsin inhibitor

Hydrogen exchange rates of six beta-sheet peptide amide protons in bovine pancreatic trypsin inhibitor (BPTI) have been measured in free BPTI and in the complexes trypsinogen-BPTI, trypsinogen-Ile-Val-BPTI, bovine trypsin-BPTI, and porcine trypsin-BPTI. Exchange rates in the complexes are slower for Ile-18, Arg-20, Gln-31, Phe-33, Tyr-35, and Phe-45 NH, but the magnitude of the effect is highly variable. The ratio of the exchange rate constant in free BPTI to the exchange rate constant in the complex, k/kcpIx, ranges from 3 to much greater than 10(3). Gln-31, Phe-45, and Phe-33 NH exchange rate constants are the same in each of the complexes. For Ile-18 and Tyr-35, k/kcpIx is much greater than 10(3) for the trypsin complexes but is in the range 14-43 for the trypsinogen complexes. Only the Arg-20 NH exchange rate shows significant differences between trypsinogen-BPTI and trypsinogen-Ile-Val-BPTI and between porcine and bovine trypsin-BPTI.     

The structure of denatured bovine pancreatic trypsin inhibitor (BPTI)

In the presence of denaturant and thiol initiator, the native bovine pancreatic trypsin inhibitor (BPTI) denatures by shuffling its native disulfide bonds and converts to a mixture of scrambled isomers. The extent of denaturation is evaluated by the relative yields of the scrambled and native species of BPTI. BPTI is an exceedingly stable molecule and can be effectively denatured only by guanidine thiocyanate (GdmSCN) at concentrations higher than 3-4 M. The denatured BPTI consists of at least eight fractions of scrambled isomers. Their composition varies under increasing concentrations of GdmSCN. In the presence of 6 M GdmSCN, the most predominant fraction of scrambled BPTI accounts for 56% of the total structure of denatured BPTI. Structural analysis reveals that this predominant fraction contains the bead-form isomer of scrambled BPTI, bridged by three pairs of neighboring cysteines, Cys5-Cys14, Cys30-Cys38 and Cys51-Cys55. The extreme conformational stability of BPTI has important implications in its distinctive folding pathway.     

The solution structure of bovine pancreatic trypsin inhibitor at high pressure

The solution structure of bovine pancreatic trypsin inhibitor (BPTI) at a pressure of 2 kbar is presented. The structure was calculated as a change from an energy-minimized low-pressure structure, using (1)H chemical shifts as restraints. The structure has changed by 0.24 A RMS, and has almost unchanged volume. The largest changes as a result of pressure are in the loop 10-16, which contains the active site of BPTI, and residues 38-42, which are adjacent to buried water molecules. Hydrogen bonds are compressed by 0.029 +/- 0.117 A, with the longer hydrogen bonds, including those to internal buried water molecules, being compressed more. The hydrophobic core is also compressed, largely from reduction of packing defects. The parts of the structure that have the greatest change are close to buried water molecules, thus highlighting the importance of water molecules as the nucleation sites for volume fluctuation of proteins in native conditions.     

Nonlocal interactions stabilize compact folding intermediates in reduced unfolded bovine pancreatic trypsin inhibitor.

To further our understanding of the protein folding process, it is desirable to examine the structural intermediates (equilibrium and kinetic) that are populated between the statistical coil state and the folded molecule. X-ray crystallography and NMR structural studies are unable to determine long-range distances in proteins under denaturing solution conditions. Nonradiative (F?rster) energy transfer, however, has been shown to be a spectroscopic ruler for the measurement of distance distributions and diffusion between selected sites in proteins under a range of different solution conditions. The distributions of distances between a donor probe at the N-terminal residue and an acceptor attached to one of the four lysine residues (15, 26, 41, 46) of reduced and unfolded (in 6 M guanidine hydrochloride and 20 mM dithiothreitol) bovine pancreatic trypsin inhibitor (BPTI) were measured as a function of temperature. Even in strong denaturant and reducing agent, BPTI does not exist as a statistical coil polypeptide. It appears that nonlocal (long-range) interactions are already beginning to "fold" the protein toward a more compact, native conformation. As the temperature is increased under these conditions, hydrophobic interactions lead to an even more compact structure consistent with the predictions of phase diagrams for globular proteins.     

Crystal structure of a Y35G mutant of bovine pancreatic trypsin inhibitor.

The structure of a Y35G mutant of bovine pancreatic trypsin inhibitor (BPTI) was solved by molecular replacement and was refined by both simulated annealing and restrained least-squares at 1.8 A resolution. The crystals belong to the space group P42212, with unit cell dimensions a = b = 46.75 A, c = 50.61 A. The final R-factor is 0.159 and the deviation from ideality for bond distances is 0.02 A. The structure of the mutant differs from that of the native protein, showing an overall root-mean-square (r.m.s.) difference of 1.86 A for main-chain atoms. However, the change is mostly localized in the two loops (respective r.m.s. values of 2.04 A and 3.93 A) and the C terminus (r.m.s. 6.79 A), while the core of the protein is well conserved (r.m.s. 0.45 A). The change in the loop regions can be clearly attributed to the mutation while the difference in the C terminus might be only due to a different crystal packing. Seventy water molecules were included in the model but only seven of them are shared with the native structure. Thermal parameters are showing a good correlation with those for the wild-type of BPTI.     

High-resolution structure of bovine pancreatic trypsin inhibitor with altered binding loop sequence

A mutant of bovine pancreatic trypsin inhibitor (BPTI) has been constructed and expressed in Escherichia coli in order to probe the kinetic and structural consequences of truncating the binding loop residues to alanine. In addition to two such mutations (Thr11Ala and Pro13Ala), it has a conservative Lys15Arg substitution at position P(1) and an unrelated Met52Leu change. In spite of the binding loop modification, the affinity for trypsin is only 30 times lower than that of the wild-type protein. At pH 7.5 the protein can be crystallized on the time-scale of hours, yielding very stable crystals of a new (tetragonal) form of BPTI. Conventional source X-ray data collected to 1.4 A at room temperature allowed anisotropic structure refinement characterized by R=0.1048. The structure reveals all 58 residues, including the complete C terminus, which is in a salt-bridge contact with the N terminus. The Cys14-Cys38 disulfide bridge is observed in two distinct chiralities. This bridge, together with an internal water molecule, contributes to the stabilization of the binding loop. The Ala mutations have only an insignificant and localized effect on the binding loop, which retains its wild-type conformation (maximum deviation of loop C(alpha) atoms of 0.7 A at Ala13). Four (instead of the typical three) additional water molecules are buried in an internal cleft and connected to the surface via a sulfate anion. Three more SO(4)(2-) anions are seen in the electron density, one of them located on a 2-fold axis. It participates in the formation of a dimeric structure between symmetry-related BPTI molecules, in which electrostatic and hydrogen bonding interactions resulting from the mutated Lys15Arg substitution are of central importance. This dimeric interaction involves direct recognition loop-recognition loop contacts, part of which are hydrophobic interactions of the patches created by the alanine mutations. Another 2-fold symmetric interaction between the BPTI molecules involves the formation of an antiparallel intermolecular beta-sheet that, together with the adjacent intramolecular beta-hairpin loops, creates a four-stranded structure.     

Renaturation of the reduced bovine pancreatic trypsin inhibitor

Refolding of the reduced pancreatic trypsin inhibitor has been investigated using thiol-disulphide exchange with various disulphide reagents to regenerate the three disulphide bonds. Essentially quantitative renaturation was routinely achieved. The refolded inhibitor was indistinguishable from the original protein in interaction with trypsin and chymotrypsin, electrophoretic mobility, and nature of disulphide bonds.The kinetics of refolding using oxidized dithiothreitol to form the disulphide bonds have been studied in some detail. The renaturation reaction is usually of second-order, being first-order in both inhibitor and disulphide reagent concentrations. A short lag period in the appearance of inhibitor activity and the inhibition of the rate, but not the extent, of renaturation by low levels of reduced dithiothreitol suggest the accumulation of metastable intermediates. In addition, heterogeneity of the refolding reaction is apparent at high concentrations of disulphide reagent, with a fraction of the material being only slowly renatured.     

Basic pancreatic trypsin inhibitor has unusual thermodynamic stability parameters

The stability parameters delta Gst, delta Hst and delta Sst of native basic pancreatic trypsin inhibitor (BPTI) have been characterized by microcalorimetric unfolding studies in various buffer solutions, at different pH values and in the presence of guanidine hydrochloride. The unfolding enthalpy of BPTI, in contrast ot other globular proteins, exhibits a very small dependence on temperature, which results in a characteristic different temperature dependence of the Gibbs energy of stabilization. BPTI has a very high specific Gibbs energy of stabilization, which renders the slow exchange rates of amide protons understandable. Comparison of the unfolding entropy of BPTI at 110 degrees C with corresponding values of other proteins, revealed that the delta S values of BPTI are lower by 2.9 J/(K X residue). This lower value of the unfolding entropy is in good agreement with predictions of a theoretical study by Poland & Scheraga (1965) where the influence of crosslinks on the configurational entropy has been studied. Additionally, we were able to calculate an interaction enthalpy per site of -5.6 kJ/mol based on the measurements of unfolding of BPTI in 6 M-guanidine hydrochloride.     

Prediction of a low-frequency mode in bovine pancreatic trypsin inhibitor molecule

One of the frontiers today in molecular biology is to measure, identify and go further to predict the low-frequency internal motion of biological macromolecules, which is crucially important for understanding the dynamic mechanism of various biological functions occurring in such molecules. Based on the theory of continuity model developed recently for dealing with the internal low-frequency motion of a biological macromolecule, it is predicted that the low-frequency phonons with wave number of about 23 cm^?1 might be excited in BPTI molecule.     

Folding pathway of a circular form of bovine pancreatic trypsin inhibitor

The pathway of unfolding and refolding of a circular form of bovine pancreatic trypsin inhibitor, in which the termini were linked together in a peptide bond, has been examined by trapping and identifying the disulphide-containing intermediates, as was done previously for the unmodified protein. The folding pathway of the circular protein was essentially the same as that of the unmodified inhibitor, although there were differences in the distribution of intermediates that accumulated and in the rates of some steps. The effects of the cross-link between the termini on the stabilities of the folding intermediates and the native state were determined by measuring the rates of the interconversions making up the folding transition, and comparing them with those measured for the unmodified protein. The major effect of the cross-link was to stabilize an intermediate containing two native disulphides, (30-51, 14-38), but lacking the disulphide nearest the termini, 5-55. The native conformation was not measurably stabilized by the cross-link, in spite of the expected reduction of entropy of the unfolded state, indicating that the native state of the circular protein had a slightly strained conformation. The stabilities of the major one-disulphide intermediates were not significantly affected by the cross-link, suggesting that the termini of bovine pancreatic trypsin inhibitor do not tend to interact during the early stage of folding.     

Structure of form III crystals of bovine pancreatic trypsin inhibitor

The structure of bovine pancreatic trypsin inhibitor has been solved in a new crystal form III. The crystals belong to space group P2(1)2(1)2 with a = 55.2 A, b = 38.2 A, c = 24.05 A. The structure was solved on the basis of co-ordinates of forms I and II of the inhibitor by molecular replacement, and the X-ray data extending to 1.7 A were used in a restrained least-squares refinement. The final R factor was 0.16, and the deviation of bonded distances from ideality was 0.020 A. Root-mean-square discrepancy between C alpha co-ordinates of forms III and I are 0.47 A, whilst between forms II and III the discrepancy is 0.39 A. These deviations are about a factor of 3 larger than the expected experimental errors, showing that true differences exist between the three crystal forms. Two residues (Arg39 and Asp50) were modeled with two positions for their side-chains. The final model includes 73 water molecules and one phosphate group bound to the protein. Sixteen water molecules occupy approximately the same positions in all three crystal forms studied to date, indicating their close association with the protein molecule. Temperature factors also show a high degree of correlation between the three crystal forms.     

Stability studies on derivatives of the bovine pancreatic trypsin inhibitor

Gibbs energy, enthalpy, and entropy data were determined for two selectively modified analogues of bovine pancreatic trypsin inhibitor (BPTI) to provide a model free set of thermodynamic parameters that characterize (a) the energetic and entropic contributions of the 14-38 disulfide bridge and (b) the variation of the overall stability resulting from the introduction of two negative charges into the positions 14 and 38. The two BPTI analogues studied were BPTI having Cys-14 and Cys-38 carboxymethylated (BPTI-RCOM) and BPTI having Cys-14 and Cys-38 carboxamidomethylated (BPTI-RCAM). They were obtained from native BPTI by reduction, followed by modification of the sulfhydryl groups with iodoacetic acid or iodoacetamide, respectively. The temperature dependence of all thermodynamic parameters of BPTI is drastically altered in the absence of the third disulfide bridge. Even the apparently minute difference of two dissociable carboxyl groups instead of uncharged amide groups in positions 14 and 38 has surprisingly large effects on the temperature dependence of the stabilization enthalpy. The Gibbs energy of BPTI at pH 2, 25 degrees C, decreases by approximately 70% when the 14-38 disulfide bond is cleaved. BPTI-RCOM is more stable than BPTI-RCAM in the whole pH range studied. The difference of -4 kJ/mol at pH 2, 25 degrees C, is reduced to -2.7 kJ/mol at pH 5, 25 degrees C. This finding demonstrates that the presence of two negative charges reduces the higher stability of BPTI-RCOM slightly; however, the overall effect of the two charges is still a stabilization.(ABSTRACT TRUNCATED AT 250 WORDS)     

Bovine pancreatic trypsin inhibitor and related isoinhibitors in bovine liver

Summary A Kunitz-type inhibitor family has been biochemically and histochemically characterized in bovine liver. This family includes the well-known pancreatic trypsin inhibitor (BPTI) and three BPTI-related molecular forms (isoinhibitors I, II and III). The purification of the inhibitors was performed by affinity chromatography on immobilized trypsin followed by fast protein liquid chromatography. The inhibitors were identical to those identified previously in bovine spleen and lung. Light immunohistochemical experiments were done by a streptavidin-biotin-peroxidase method using two different immunoglobulin preparations, which selectively discriminated between BPTI and the other isoinhibitors. BPTI-related immunoreactivity was found exclusively at the level of isolated cells, of which many were identified as mast cells by toluidine blue staining. By contrast, isoinhibitor-related immunoreactivity showed a more widespread distribution, including hepatocytes, mast cells and biliary duct epithelial cells. Finally, specific immunoreactivity was also present in plasma. These results suggest that: i) BPTI and related isoinhibitors may be involved in the regulation of the activity of some mast cell proteases, as it happens in other bovine organs (Businaro et al. 1987, 1988); ii) BPTI isoinhibitors, but not BPTI itself, may also control proteolytic activities in hepatic specific structures (hepatocytes and biliary duct epithelial cells).     

Folding of the twisted beta-sheet in bovine pancreatic trypsin inhibitor

The dominant role of local interactions has been demonstrated for the formation of the strongly twisted antiparallel beta-sheet structure consisting of residues 18-35 in bovine pancreatic trypsin inhibitor. Conformational energy minimization has indicated that this beta-sheet has a strong twist even in the absence of the rest of the protein molecule. The twist is maintained essentially unchanged when energy minimization is carried out by starting from the native conformation. By starting from a nontwisted beta-sheet conformation of residues 18-35, a strongly twisted structure (higher in energy than the native) is obtained. The high twist of the native-like beta-sheet is a consequence of its amino acid sequence, but it is enhanced strongly by interchain interactions that operate within the beta-sheet. The existence of the twisted beta-sheet structure does not require the presence of a disulfide bond between residue 14 and residue 38. It actually may facilitate the formation of this bond. Therefore, it is likely that the beta-sheet structure forms during an earlier stage of folding than the formation of this disulfide bond. This study provides an example of the manner in which conformational energy calculations can be used to provide information about the probable pathway of the folding of a protein.     

Structure of the complex formed by bovine trypsin and bovine pancreatic trypsin inhibitor. Crystal structure determination and stereochemistry of the contact region

The structure of the complex of bovine trypsin and bovine pancreatic trypsin inhibitor has been determined by crystal structure analysis at 2.8 Å resolution. The structure is closely similar to the model predicted from the structures of the components. The complex is a tetrahedral adduct with a covalent bond between the carbonyl carbon of Lys-15I of the inhibitor and the γ-oxygen of Ser-195 of the enzyme. The imidazole of His-57 is hydrogen-bonded to Asp-102 and the bound seryl γ-oxygen in accord with the histidine being charged. The negatively charged carbonyl oxygen of Lys-15I forms two hydrogen bonds with the amide nitrogens of Gly-193 and Ser-195. Protonation of the leaving group N-H of Ala-16I to form an acyl-complex requires a conformational change of the imidazole of His-57. The tetrahedral adduct is further stabilized by hydrogen bonds between groups at the leaving group side and inhibitor and enzyme, which would be weakened in the acyl-enzyme. The kinetic data of inhibitor-enzyme interaction are reconciled with the structural model, and relations between enzyme-inhibitor interaction and productive enzyme-substrate interaction are proposed.