Mechanism of surface peptide proton exchange in bovine pancreatic trypsin inhibitor. Salt effects and O-protonation

The acid-catalyzed hydrogen exchange rate constants kH, and the base-catalyzed rate constants kOH, have been determined (in the preceding paper) for the 25 most rapidly exchanging NH groups of bovine pancreatic trypsin inhibitor. Most of these NH groups are at the protein-solvent interface. The correlation of kH, but not kOH, with the static accessibility and hydrogen bonding of the peptide carbonyl O atom indicates that the mechanism of acid catalysis in proteins involves O-protonation. Agreement between the ionic strength dependence observed for kH and kOH and the ionic strength dependence calculated for an O-protonation mechanism supports this conclusion. N-protonation for acid catalysis, as well as N-deprotonation for base catalysis, have traditionally been assumed in the mechanism of the chemical step in peptide amide proton exchange. A preference for the alternative O-protonation mechanism has far-reaching implications in the interpretation of protein hydrogen exchange kinetics. With an O-protonation mechanism, acid-catalyzed rates of surface NH groups are primarily a function of the average solvent accessibility of the carbonyl O atoms in the dynamic solution structure, while base-catalyzed rates of surface NH groups measure solvent accessibility of the peptide N. The relative dynamic accessibilities of peptide O atoms, as measured by relative values of kH (corrected for electrostatic effects), correlate with O static accessibilities in the crystal structure. A lower correlation of static accessibility of N atoms with kOH is observed for surface NH groups in peptide groups in which the carbonyl O is not hydrogen bonded. For some surface NH groups, the observed pH of minimum rate, pHmin, deviates widely from the pHmin of model compounds. This is explained as the combined result of electrostatic effects and of the differences in accessibility of the carbonyl O and N atoms that result in a change in the relative values of kH and kOH as compared to those of model peptides. A mechanism whereby exchange of interior sites is catalyzed by interactions of catalysis ions with protein surface atoms via charge transfer is suggested.     

Bovine serum albumin observed by infrared spectrometry. II. Hydration mechanisms and interaction configurations of embedded H(2)O molecules

The hydration mechanism of bovine serum albumin (BSA) is studied, and we analyze (de)hydration spectra displayed previously. We first determine the three elementary (de)hydration spectra on which all these (de)hydration spectra can be decomposed. They correspond to three different hydration mechanisms for the protein, which we define after a quantitative analysis performed in a second step. The first mechanism, which involves ionization of carboxylic COOH groups, occurs at low hydration levels and rapidly reaches a plateau when the hygroscopy is increased. It is a mechanism that involves a single H(2)O molecule and consequently requires somewhat severe steric conditions. The second mechanism occurs at all hydration levels and, because it involves more H(2)O molecules, requires less severe steric conditions. It consists of the simultaneous hydration of one amide N--H group and one carbonyl-amide C=O group by four H(2)O molecules and one carboxyl COO(-) group by eight H(2)O molecules. The third mechanism is simpler and consists of the introduction of H(2)O molecules into the hydrogen-bond network of the hydrated protein. It becomes important at a high hydration level, when the presence of an appreciable number of H(2)O molecules makes this hydrogen-bond network well developed. This analysis also shows that 80 H(2)O molecules remain embedded in one dried protein made of 604 peptide units. They are held by hydrogen bonds established by N--H groups and at the same time they establish two hydrogen bonds on two carbonyl-amide C=O groups. The proportion of free N--H groups can be determined together with that of carbonyl-amide C=O groups accepting no hydrogen bonds and that of carbonyl-amide C=O groups accepting two hydrogen bonds. The proportion of N--H groups establishing one hydrogen bond directly on a carbonyl-amide C=O group is 65%, which is the proportion of peptide units found in alpha helices in BSA.     

Hydration of oligonucleotides in crystals

The solvent molecules found around crystallized oligonucleotides after X-ray refinement are analysed in terms of interaction sites to bases, phosphates and sugars in the three main forms of nucleic acid structures, the A-form, the B-form and the Z-form. The average numbers of contacts to nucleic acid atoms made by solvent molecules are identical in the three forms, but it appears that the average number of contacts solvent molecules make with each other depends on the resolution of the structure. The phosphate anionic oxygen atoms are the most hydrated, while the O(3′) and O(5′) backbone atoms and the ring oxygen atom O(4′) are the least hydrated. Among the hydrophilic atoms of the bases, there is a modulation of the relative water affinities with the nucleic acid form. Numerous hydration sites are such that water molecules can bridge hydrophilic atoms of the same residue, of adjacent residues on the same strand, of distant residues on the two strands, or belonging to symmetry-related residues. Through the helical periodicity of the nucleic acid structure, those bridges can lead to regular and striking hydration networks involving several water molecules and characteristic of the nucleic acid form. Solvent dynamics, as seen by temperature factor versus occupancy plots, seems intimately related to nucleic acid structure and dynamics, since they depend on hydration sites around the nucleic acids.     

Hydration of amino acid side chains: dependence on secondary structure.

Energy calculations have been used to study the hydration sites around the polar groups of serine, threonine and tyrosine side chains. These hydration sites depend not only on the hybridization of the polar group but also on the local secondary structure, the chi 1 side chain torsion angle and the position of the hydroxyl hydrogen atom. For tyrosine side chains, two solvent sites are found approximately in the plane of the ring. Even for serine and threonine side chains only two minimum energy sites are found in general of which one is in an expected position within hydrogen bonding of the hydroxyl hydrogen atom (unless this is blocked from interaction with solvent molecules by, for example, Oi-4 or Oi-3. The position of the second of these sites depends not only on the position of the hydroxyl oxygen but also on neighbouring main chain atoms to which it can also hydrogen bond. There is good agreement with the solvent distributions obtained from crystallographic data.     

Structure of rubredoxin from Desulfovibrio vulgaris at 1.5 A resolution

The X-ray model of rubredoxin from Desulfovibrio vulgaris has been refined against 1.5 A X-ray diffraction data collected on a diffractometer. The final model comprises 395 non-hydrogen protein atoms, and 180 solvent O atoms. The final R-value for the model with calculated H atom positions included as fixed contributions is 0.098 over all reflections greater than 2 sigma I from infinity to 1.5 A. The error in co-ordinates is estimated to be 0.08 A. The solvent model was twice redetermined during the later stages of refinement and was instrumental in its success. One sequence error has been detected and corrected (Thr21----Asp). The iron-sulfur site bond angles are distorted from true tetrahedral symmetry, as found in other rubredoxin structures. A significant deviation from tetrahedral angles is seen at C alpha atoms 9, 10, 42 and 43, interior angles of the loops binding the iron atom. The planes of two aromatic groups, Tyr4 and Trp37, are nearly parallel to, and lie under, an extended system of atoms that includes the peptide bonds preceding the first cysteine residue of each cysteine loop as well as the cysteine side-chain, the iron, and the cysteine side-chain of the opposite loop, forming a previously unrecognized extended system that may function in electron transfer.     

The molecular basis of the temperature- and pH-induced conformational transitions in elastin-based peptides

Elastin undergoes an inverse temperature transition and collapses at high temperatures in both simulation and experiment. We investigated a pH-dependent modification of this transition by simulating a glutamic acid (Glu)-substituted elastin at varying pHs and temperatures. The Glu-substituted peptide collapsed at higher temperature than the unsubstituted elastin when Glu was charged. The charge effects could be reversed by neutralization of the Glu carboxyl groups at low pH, and in that case the peptide collapsed at a lower temperature. The collapse was accompanied by the formation of beta-turns and short distorted beta-sheets. Formation of contacts between hydrophobic side chains drives the collapse at high temperature, but interactions between water and polar groups (Glu and main chain) can attenuate this effect at high pH. The overall competition and balance of the polar and nonpolar groups determined the conformational states of the peptide. Water hydration contributed to the conformational transition, and the peptide and its hydration shell must be considered. Structurally, waters near polar residues mainly formed hydrogen bonds with the protein atoms, while waters around the hydrophobic side chains tended to be parallel to the peptide groups to maximize water-water interactions.     

X-ray crystal structures of the oxidized and reduced forms of the rubredoxin from the marine hyperthermophilic archaebacterium Pyrococcus furiosus.

The structures of the oxidized and reduced forms of the rubredoxin from the archaebacterium, Pyrococcus furiosus, an organism that grows optimally at 100 degrees C, have been determined by X-ray crystallography to a resolution of 1.8 A. Crystals of this rubredoxin grow in space group P2(1)2(1)2(1) with room temperature cell dimensions a = 34.6 A, b = 35.5 A, and c = 44.4 A. Initial phases were determined by the method of molecular replacement using the oxidized form of the rubredoxin from the mesophilic eubacterium, Clostridium pasteurianum, as a starting model. The oxidized and reduced models of P. furiosus rubredoxin each contain 414 nonhydrogen protein atoms comprising 53 residues. The model of the oxidized form contains 61 solvent H2O oxygen atoms and has been refined with X-PLOR and TNT to a final R = 0.178 with root mean square (rms) deviations from ideality in bond distances and bond angles of 0.014 A and 2.06 degrees, respectively. The model of the reduced form contains 37 solvent H2O oxygen atoms and has been refined to R = 0.193 with rms deviations from ideality in bond lengths of 0.012 A and in bond angles of 1.95 degrees. The overall structure of P. furiosus rubredoxin is similar to the structures of mesophilic rubredoxins, with the exception of a more extensive hydrogen-bonding network in the beta-sheet region and multiple electrostatic interactions (salt bridge, hydrogen bonds) of the Glu 14 side chain with groups on three other residues (the amino-terminal nitrogen of Ala 1; the indole nitrogen of Trp 3; and the amide nitrogen group of Phe 29). The influence of these and other features upon the thermostability of the P. furiosus protein is discussed.     

The 1.9 Å crystal structure of the “as isolated” rubrerythrin from <Emphasis Type="Italic">Desulfovibrio vulgaris</Emphasis>: some surprising results

Rubrerythrin is a non-heme iron dimeric protein isolated from the sulfate-reducing bacterium Desulfovibrio vulgaris. Each monomer has one mononuclear iron center similar to rubredoxin and one dinuclear metal center similar to hemerythrin or ribonucleotide reductase. The 1.88 A X-ray structure of the "as isolated" molecule and a uranyl heavy atom derivative have been solved by molecular replacement techniques. The resulting model of the native "as isolated" molecule, including 164 water molecules, has been refined giving a final R factor of 0.197 (R(free) = 0.255). The structure has the same general protein fold, domain structure, and dimeric interactions as previously found for rubrerythrin [1, 2], but it also has some interesting undetected differences at the metal centers. The refined model of the protein structure has a cis peptide between residues 78 and 79. The Fe-Cys4 center has a previously undetected strong seventh N-H...S hydrogen bond in addition to the six N-H...S bonds usually found in rubredoxin. The dinuclear metal center has a hexacoordinate Fe atom and a tetracoordinate Zn atom. Each metal is coordinated by a GluXXHis polypeptide chain segment. The Zn atom binds at a site distinctly different from that found in the structure of a diiron rubrerythrin. Difference electron density for the uranyl derivative shows an extremely large peak adjacent to and replacing the Zn atom, indicating that this particular site is capable of binding other atoms. This feature/ability may give rise to some of the confusing activities ascribed to this molecule.     

Conformational features of a hexapeptide model Ac-TGAAKA-NH2 corresponding to a hydrated alpha helical segment from glyceraldehyde 3-phosphate dehydrogenase: implications for the role of turns in helix folding

Recent analysis of alpha helices in protein crystal structures, available in literature, revealed hydrated alpha helical segments in which, water molecule breaks open helix 5-->1 hydrogen bond by inserting itself, hydrogen bonds to both C=O and NH groups of helix hydrogen bond without disrupting the helix hydrogen bond, and hydrogen bonds to either C=O or NH of helix hydrogen bond. These hydrated segments display a variety of turn conformations and are thought to be 'folding intermediates' trapped during folding-unfolding of alpha helices. A role for reverse turns is implicated in the folding of alpha helices. We considered a hexapeptide model Ac-1TGAAKA6-NH2 from glyceraldehyde 3-phosphate dehydrogenase, corresponding to a hydrated helical segment to assess its role in helix folding. The sequence is a site for two 'folding intermediates'. The conformational features of the model peptide have been investigated by 1H 2D NMR techniques and quantum mechanical perturbative configuration interaction over localized orbitals (PCILO) method. Theoretical modeling largely correlates with experimental observations. Based upon the amide proton temperature coefficients, the observed d alpha n(i, i + 1), d alpha n(i, i + 2), dnn(i, i + 1), d beta n(i, i + 1) NOEs and the results from theoretical modeling, we conclude that the residues of the peptide sample alpha helical and neck regions of the Ramachandran phi, psi map with reduced conformational entropy and there is a potential for turn conformations at N and C terminal ends of the peptide. The role of reduced conformational entropy and turn potential in helix formation have been discussed. We conclude that the peptide sequence can serve as a 'folding intermediate' in the helix folding of glyceraldehyde 3-phosphate dehydrogenase.     

A rare polyglycine type II‐like helix motif in naturally occurring proteins

Common structural elements in proteins such as α‐helices or β‐sheets are characterized by uniformly repeating, energetically favorable main chain conformations which additionally exhibit a completely saturated hydrogen‐bonding network of the main chain NH and CO groups. Although polyproline or polyglycine type II helices (PP_II or PG_II) are frequently found in proteins, they are not considered as equivalent secondary structure elements because they do not form a similar self‐contained hydrogen‐bonding network of the main chain atoms. In this context our finding of an unusual motif of glycine‐rich PG_II‐like helices in the structure of the acetophenone carboxylase core complex is of relevance. These PG_II‐like helices form hexagonal bundles which appear to fulfill the criterion of a (largely) saturated hydrogen‐bonding network of the main‐chain groups and therefore may be regarded in this sense as a new secondary structure element. It consists of a central PG_II‐like helix surrounded by six nearly parallel PG_II‐like helices in a hexagonal array, plus an additional PG_II‐like helix extending the array outwards. Very related structural elements have previously been found in synthetic polyglycine fibers. In both cases, all main chain NH and CO groups of the central PG_II‐helix are saturated by either intra‐ or intermolecular hydrogen‐bonds, resulting in a self‐contained hydrogen‐bonding network. Similar, but incomplete PG_II‐helix patterns were also previously identified in a GTP‐binding protein and an antifreeze protein.     

Effects of hydrated water on protein unfolding

The conformational stability of a protein in aqueous solution is described in terms of the thermodynamic properties such as unfolding Gibbs free energy, which is the difference in the free energy (Gibbs function) between the native and random conformations in solution. The properties are composed of two contributions, one from enthalpy due to intramolecular interactions among constituent atoms and chain entropy of the backbone and side chains, and the other from the hydrated water around a protein molecule. The hydration free energy and enthalpy at a given temperature for a protein of known three-dimensional structure can be calculated from the accessible surface areas of constituent atoms according to a method developed recently. Since the hydration free energy and enthalpy for random conformations are computed from those for an extended conformation, the thermodynamic properties of unfolding are evaluated quantitatively. The evaluated hydration properties for proteins of known transition temperature (Tm) and unfolding enthalpy (delta Hm) show an approximately linear dependence on the number of constituent heavy atoms. Since the unfolding free energy is zero at Tm, the enthalpy originating from interatomic interactions of a polypeptide chain and the chain entropy are evaluated from an experimental value of delta Hm and computed properties due to the hydrated water around the molecule at Tm. The chain enthalpy and entropy thus estimated are largely compensated by the hydration enthalpy and entropy, respectively, making the unfolding free energy and enthalpy relatively small. The computed temperature dependences of the unfolding free energy and enthalpy for RNase A, T4 lysozyme, and myoglobin showed a good agreement with the experimental ones.(ABSTRACT TRUNCATED AT 250 WORDS)     

Hydration in proteins observed by high-resolution neutron crystallography

It is well known that water molecules surrounding a protein play important roles in maintaining its structural stability. Water molecules are known to participate in several physiological processes through the formation of hydrogen bonds. However, the hydration structures of most proteins are not known well at an atomic level at present because X-ray protein crystallography has difficulties to localize hydrogen atoms. In contrast, neutron crystallography has no problem in determining the position of hydrogens with high accuracy.1 In this article, the hydration structures of three proteins are described- myoglobin, wild-type rubredoxin, and a mutant rubredoxin-the structures of which were solved at 1.5- or 1.6-A resolution by neutron structure determination. These hydration patterns show fascinating features and the water molecules adopt a variety of shapes in the neutron Fourier maps, revealing details of intermolecular hydrogen bond formation and dynamics of hydration. Our results further show that there are strong relationships between these shapes and the water environments.     

Study of the structure of N-acyldipalmitoylphosphatidylethanolamines in aqueous dispersion by infrared and Raman spectroscopies

The effect of the headgroup chain length on the structure and on the thermotropic behavior of N-acyldipalmitoylphosphatidylethanolamines (N-acyl-DPPEs) has been studied by infrared and Raman spectroscopies. The results show that the N-acyl-DPPEs can be divided in two classes depending on the N-acyl chain length. When the N-acyl chain contains 10 carbon atoms or more, it penetrates into the bilayer while it remains at the level of the glycerol backbone for shorter N-acyl chains. For both classes of N-acyl-DPPEs, the rotation of the lipid chains in the liquid-crystalline phase is hindered by the presence of the N-acyl group. In addition, the disruption of the hydrogen bonds between the amino and phosphate groups by N-acylation of the amino group results in an increase of the hydration of the phosphate group compared to that in DPPE. The hydration occurred at both the phosphate and amide group levels; the phosphate group is more hydrated for phospholipids with long N-acyl chains while in the case of short-chain derivatives both the phosphate and amide groups are hydrated. This higher degree of hydration coupled with the immobilization of the lipid molecule may contribute to the bilayer stabilizer role of N-acyl-PEs since hydration is an important factor in bilayer stability.     

The environment of amide groups in protein–ligand complexes: H-bonds and beyond

A comprehensive structural analysis of interactions involving amide NH and C=O groups in protein-ligand complexes has been performed based on 3,275 published crystal structures (resolution < or =2.5 A). Most of the amide C=O and NH groups at the protein-ligand interface are highly buried within the binding site and involved in H-bonds with corresponding counter-groups. Small percentages of C=O and NH groups are solvated or embedded in hydrophobic environments. In particular, C=O groups show a higher propensity to be solvated or embedded in a hydrophobic environment than NH groups do. A small percentage of carbonyl groups is involved in weak hydrogen bonds with CH. Cases of dipolar interactions, involving carbonyl oxygen and electrophilic carbon atoms, such as amide, amidinium, guanidium groups, are also identified. A higher percentage of NH are in contact with aromatic carbons, interacting either through hydrogen bonds (preferably with the NH group pointing towards a ring carbon atom) or through stacking between amide plane and ring plane. Comprehensive studies such as the present one are thought to be important for future improvements in the molecular design area, in particular for the development of new scoring functions. [Figure: see text].     

Patterns in ionizable side chain interactions in protein structures

In a selected set of 44 high-resolution, non-homologous protein structures, the intramolecular hydrogen bonds or salt bridges formed by ionizable amino acid side chains were identified and analyzed. The analysis was based on the investigation of several properties of the involved residues such as their solvent exposure, their belonging to a certain secondary structural element, and their position relative to the N- and C-termini of their respective structural element. It was observed that two-thirds of the interactions made by basic or acidic side chains are hydrogen bonds to polar uncharged groups. In particular, the majority (78%) of the hydrogen bonds between ionizable side chains and main chain polar groups (sch:mch bonds) involved at least one buried atom, and in 42% of the cases both interacting atoms were buried. In α-helices, the sch:mch bonds observed in the proximity of the C- and N-termini show a clear preference for acidic and basic side chains, respectively. This appears to be due to the partial charges of peptide group atoms at the termini of α-helices, which establish energetically favorable electrostatic interactions with side chain carrying opposite charge, at distances even greater than 4.5 Å. The sch:mch interactions involving ionizable side chains that belong either to β-strands or to the central part of α-helices are based almost exclusively on basic residues. This results from the presence of main chain carbonyl oxygen atoms in the protein core which have unsatisfied hydrogen bonding capabilities.     

Crystal structure of oxidized flavodoxin from a red alga Chondrus crispus refined at 1.8 A resolution. Description of the flavin mononucleotide binding site.

In order to describe the detailed conformation of the oxidized flavodoxin from a eukaryotic red alga, Chondrus crispus, the crystal structure has been refined by a restrained least-squares method. The crystallographic R factor is 0.168 for 13,899 reflections with F greater than 2 sigma F between 6.0 and 1.8 A resolution. The refined model includes 173 amino acid residues, flavin mononucleotide (FMN) and 110 water molecules. The root-mean-square deviation in bond lengths from ideal values is 0.015 A, and the mean co-ordinate error is estimated to be 0.2 A. The FMN is located at the periphery of the molecule. The orientation of the isoalloxazine ring is such that the C-7 and C-8 methyl groups are exposed to solvent and the pyrimidine moiety is buried in the protein. Three peptide segments, T8-T13, T55-T58 and D94-C103, are involved in FMN binding. The first segment of T8-T13 enfolds the phosphate group of the FMN. The three oxygen atoms in the phosphate group form extensive hydrogen bonds with amide groups of the main chain and the O gamma atoms of the side-chains in this segment. T55 O and W56 N epsilon 1 in the second segment form hydrogen bonds with O-2 in the ribityl moiety and one of the oxygen atoms in the phosphate group, respectively. The O gamma H of T58 forms a hydrogen bond with the N-5 atom in the isoalloxazine ring, which is expected to be protonated in the semiquinone form. The third segment is in contact with the isoalloxazine ring. It appears that the hydrogen bond acceptor of the NH of Asp94 in the third segment is O-2 rather than N-1 in the isoalloxazine ring. The isoalloxazine ring is flanked by the side-chains of Trp56 and Tyr98; it forms an angle of 38 degrees with the indole ring of Trp56 and is almost parallel to the benzene ring of Tyr98. The environment of the phosphate group is conserved as in other flavodoxins whereas that of the isoalloxazine ring differs. The relationship between the hydrogen bond to the N-5 in the ring and the redox potential for the oxidized/semiquinone couple is discussed.     

Crystal structure of rubredoxin from Desulfovibrio gigas to ultra-high 0.68 A resolution

Rubredoxin (D.g. Rd) is a small non-heme iron-sulfur protein shown to function as a redox coupling protein from the sulfate reducing bacteria Desulfovibrio gigas. The protein is generally purified from anaerobic bacteria in which it is thought to be involved in electron transfer or exchange processes. Rd transfers an electron to oxygen to form water as part of a unique electron transfer chain, composed by NADH:rubredoxin oxidoreductase (NRO), rubredoxin and rubredoxin:oxygen oxidoreductase (ROO) in D.g. The crystal structure of D.g. Rd has been determined by means of both a Fe single-wavelength anomalous dispersion (SAD) signal and the direct method, and refined to an ultra-high 0.68 A resolution, using X-ray from a synchrotron. Rd contains one iron atom bound in a tetrahedral coordination by the sulfur atoms of four cysteinyl residues. Hydrophobic and pi-pi interactions maintain the internal Rd folding. Multiple conformations of the iron-sulfur cluster and amino acid residues are observed and indicate its unique mechanism of electron transfer. Several hydrogen bonds, including N-H...SG of the iron-sulfur, are revealed clearly in maps of electron density. Abundant waters bound to C-O peptides of residues Val8, Cys9, Gly10, Ala38, and Gly43, which may be involved in electron transfer. This ultrahigh-resolution structure allows us to study in great detail the relationship between structure and function of rubredoxin, such as salt bridges, hydrogen bonds, water structures, cysteine ligands, iron-sulfur cluster, and distributions of electron density among activity sites. For the first time, this information will provide a clear role for this protein in a strict anaerobic bacterium.     

Solvent exchange of buried water and hydrogen exchange of peptide NH groups hydrogen bonded to buried waters in bovine pancreatic trypsin inhibitor

Solvent exchange of 18O-labeled buried water in bovine pancreatic trypsin inhibitor (BPTI), trypsin, and trypsin-BPTI complex is measured by high-precision isotope ratio mass spectrometry. Buried water is labeled by equilibration of the protein in 18O-enriched water. Protein samples are then rapidly dialyzed against water of normal isotope composition by gel filtration and stored. The exchangeable 18O label eluting with the protein in 10-300 s is determined by an H2O-CO2 equilibration technique. Exchange of buried waters with solvent water is complete before 10-15 s in BPTI, trypsin, and BPTI-trypsin, as well as in lysozyme and carboxypeptidase measured as controls. When in-exchange dialysis and storage are carried out at pH greater than or equal to 2.5, trypsin-BPTI and trypsin, but not free BPTI, have the equivalent of one 18O atom that exchanges slowly (after 300 s and before several days). This oxygen is probably covalently bound to a specific site in trypsin. When in-exchange dialysis and storage are carried out at pH 1.1, the equivalent of three to seven 18O atoms per molecule is associated with the trypsin-BPTI complex, apparently due to nonspecific covalent 18O labeling of carboxyl groups at low pH. In addition to 18O exchange of buried waters, the hydrogen isotope exchange of buried NH groups H bonded to buried waters was also measured. Their base-catalyzed exchange rate constants are on the order of NH groups that in the crystal are exposed to solvent (static accessibility greater than 0) and hydrogen-bonded main chain O, and their pH min is similar to that for model compounds. The pH dependence of their exchange rate constants suggests that direct exchange with water may significantly contribute to their observed exchange rate.     

Peptide--water association in peptide crystals.

The structures of 37 peptide crystals, containing 78 water-peptide hydrogen bonds and 77 other hydrogen bonds involving water, were surveyed to identify the geometry of peptide backbone hydration. In the sample, hydration of peptide carbonyl occurred more frequently than hydration of peptide N--H. The most probable value of the C'=O ... O water angle was near 138 degrees, considerably greater than the 120 degrees to the axis of a lone electron pair on the carbonyl oxygen. Associated water oxygens tended to be in the plane of the peptide bond, bui--H and Ci+1=O atoms, was common in glycine-containing cyclic hexapeptides. The distribution of angles between two hydrogen bonds at a single water molecule, as defined by the three nonhydrogen atoms involved, was centered near the tetrahedral angle.