Strong Ionic Hydrogen Bonding Causes a Spectral Isotope Effect in Photoactive Yellow Protein

Standard hydrogen bonds are of great importance for protein structure and function. Ionic hydrogen bonds often are significantly stronger than standard hydrogen bonds and exhibit unique properties, but their role in proteins is not well understood. We report that hydrogen/deuterium exchange causes a redshift in the visible absorbance spectrum of photoactive yellow protein (PYP). We expand the range of interpretable isotope effects by assigning this spectral isotope effect (SIE) to a functionally important hydrogen bond at the active site of PYP. The inverted sign and extent of this SIE is explained by the ionic nature and strength of this hydrogen bond. These results show the relevance of ionic hydrogen bonding for protein active sites, and reveal that the inverted SIE is a novel, to our knowledge, tool to probe ionic hydrogen bonds. Our results support a classification of hydrogen bonds that distinguishes the properties of ionic hydrogen bonds from those of both standard and low barrier hydrogen bonds, and show how this classification helps resolve a recent debate regarding active site hydrogen bonding in PYP.     

Strong Ionic Hydrogen Bonding Causes a Spectral Isotope Effect in Photoactive Yellow Protein

Standard hydrogen bonds are of great importance for protein structure and function. Ionic hydrogen bonds often are significantly stronger than standard hydrogen bonds and exhibit unique properties, but their role in proteins is not well understood. We report that hydrogen/deuterium exchange causes a redshift in the visible absorbance spectrum of photoactive yellow protein (PYP). We expand the range of interpretable isotope effects by assigning this spectral isotope effect (SIE) to a functionally important hydrogen bond at the active site of PYP. The inverted sign and extent of this SIE is explained by the ionic nature and strength of this hydrogen bond. These results show the relevance of ionic hydrogen bonding for protein active sites, and reveal that the inverted SIE is a novel, to our knowledge, tool to probe ionic hydrogen bonds. Our results support a classification of hydrogen bonds that distinguishes the properties of ionic hydrogen bonds from those of both standard and low barrier hydrogen bonds, and show how this classification helps resolve a recent debate regarding active site hydrogen bonding in PYP.     

Hydrogen-bond disruption probability in proteins by a modified self-consistent harmonic approach

Modified self-consistent harmonic approach was employed to calculate the probability for the disruption of each individual hydrogen bonds (H bonds) in x-ray crystal structure of several proteins. The computed probability for 82% of intraprotein and water-protein H bonds studied were found to be roughly consistent with estimated free energies from protein engineering and hydrogen exchange experiments. Hydrogen bonds have been proposed as part of a stereochemical code for protein folding. Proteins fold into unique three-dimensional structures; therefore those bonds involved in the folding code are expected to be stable. We have applied this method to tens of hydrogen bonds in a protein assumed to be involved in the folding code of a protein. 58% of these H bonds were found to have a lower disruption probability (-1.8 kcal/mol). Our results showed that modified self-consistent harmonic approach might be explored as a method supplement to existing methods in analysis of hydrogen bonds in proteins.     

Hydrogen bonding in globular proteins.

A global census of the hydrogen bonds in 42 X-ray-elucidated proteins was taken and the following demographic trends identified: (1) Most hydrogen bonds are local, i.e. between partners that are close in sequence, the primary exception being hydrogen-bonded ion pairs. (2) Most hydrogen bonds are between backbone atoms in the protein, an average of 68%. (3) All proteins studied have extensive hydrogen-bonded secondary structure, an average of 82%. (4) Almost all backbone hydrogen bonds are within single elements of secondary structure. An approximate rule of thirds applies: slightly more than one-third (37%) form i----i--3 hydrogen bonds, almost one-third (32%) form i----i--4 hydrogen bonds, and slightly less than one-third (26%) reside in paired strands of beta-sheet. The remaining 5% are not wholly within an individual helix, turn or sheet. (5) Side-chain to backbone hydrogen bonds are clustered at helix-capping positions. (6) An extensive network of hydrogen bonds is present in helices. (7) To a close approximation, the total number of hydrogen bonds is a simple function of a protein's helix and sheet content. (8) A unique quantity, termed the reduced number of hydrogen bonds, is defined as the maximum number of hydrogen bonds possible when every donor:acceptor pair is constrained to be 1:1. This quantity scales linearly with chain length, with 0.71 reduced hydrogen bond per residue. Implications of these results for pathways of protein folding are discussed.     

Are aromatic carbon donor hydrogen bonds linear in proteins?

Proteins fold and maintain structure through the collective contributions of a large number of weak, noncovalent interactions. The hydrogen bond is one important category of forces that acts on very short distances. As our knowledge of protein structure continues to expand, we are beginning to appreciate the role that weak carbon-donor hydrogen bonds play in structure and function. One property that differentiates hydrogen bonds from other packing forces is propensity for forming a linear donor-hydrogen-acceptor orientation. To ascertain if carbon-donor hydrogen bonds are able to direct acceptor linearity, we surveyed the geometry of interactions specifically involving aromatic sidechain ring carbons in a data set of high resolution protein structures. We found that while donor-acceptor distances for most carbon donor hydrogen bonds were tighter than expected for van der Waals packing, only the carbons of histidine showed a significant bias for linear geometry. By categorizing histidines in the data set into charged and neutral sidechains, we found only the charged subset of histidines participated in linear interactions. B3LYP/6-31G**++ level optimizations of imidazole and indole-water interactions at various fixed angles demonstrates a clear orientation dependence of hydrogen bonding capacity for both charged and neutral sidechains. We suggest that while all aromatic carbons can participate in hydrogen bonding, only charged histidines are able to overcome protein packing forces and enforce linear interactions. The implications for protein modeling and design are discussed.     

The Role of Backbone Hydrogen Bonds in the Transition State for Protein Folding of a PDZ Domain

Backbone hydrogen bonds are important for the structure and stability of proteins. However, since conventional site-directed mutagenesis cannot be applied to perturb the backbone, the contribution of these hydrogen bonds in protein folding and stability has been assessed only for a very limited set of small proteins. We have here investigated effects of five amide-to-ester mutations in the backbone of a PDZ domain, a 90-residue globular protein domain, to probe the influence of hydrogen bonds in a β-sheet for folding and stability. The amide-to-ester mutation removes NH-mediated hydrogen bonds and destabilizes hydrogen bonds formed by the carbonyl oxygen. The overall stability of the PDZ domain generally decreased for all amide-to-ester mutants due to an increase in the unfolding rate constant. For this particular region of the PDZ domain, it is therefore clear that native hydrogen bonds are formed after crossing of the rate-limiting barrier for folding. Moreover, three of the five amide-to-ester mutants displayed an increase in the folding rate constant suggesting that the hydrogen bonds are involved in non-native interactions in the transition state for folding.     

An energetic scale for equilibrium H/D fractionation factors illuminates hydrogen bond free energies in proteins

Equilibrium H/D fractionation factors have been extensively employed to qualitatively assess hydrogen bond strengths in protein structure, enzyme active sites, and DNA. It remains unclear how fractionation factors correlate with hydrogen bond free energies, however. Here we develop an empirical relationship between fractionation factors and free energy, allowing for the simple and quantitative measurement of hydrogen bond free energies. Applying our empirical relationship to prior fractionation factor studies in proteins, we find: [1] Within the folded state, backbone hydrogen bonds are only marginally stronger on average in α‐helices compared to β‐sheets by ～0.2 kcal/mol. [2] Charge‐stabilized hydrogen bonds are stronger than neutral hydrogen bonds by ～2 kcal/mol on average, and can be as strong as –7 kcal/mol. [3] Changes in a few hydrogen bonds during an enzyme catalytic cycle can stabilize an intermediate state by –4.2 kcal/mol. [4] Backbone hydrogen bonds can make a large overall contribution to the energetics of conformational changes, possibly playing an important role in directing conformational changes. [5] Backbone hydrogen bonding becomes more uniform overall upon ligand binding, which may facilitate participation of the entire protein structure in events at the active site. Our energetic scale provides a simple method for further exploration of hydrogen bond free energies.     

Statistical and molecular dynamics studies of buried waters in globular proteins

Buried solvent molecules are common in the core of globular proteins and contribute to structural stability. Folding necessitates the burial of polar backbone atoms in the protein core, whose hydrogen-bonding capacities should be satisfied on average. Whereas the residues in alpha-helices and beta-sheets form systematic main-chain hydrogen bonds, the residues in turns, coils and loops often contain polar atoms that fail to form intramolecular hydrogen bonds. The statistical analysis of 842 high resolution protein structures shows that well-resolved, internal water molecules preferentially reside near residues without alpha-helical and beta-sheet secondary structures. These buried waters most often form primary hydrogen bonds to main-chain atoms not involved in intramolecular hydrogen bonds, providing strong evidence that hydrating main-chain atoms is a key structural role of buried water molecules. Additionally, the average B-factor of protein atoms hydrogen-bonded to waters is smaller than that of protein atoms forming intramolecular hydrogen bonds, and the average B-factor of water molecules involved in primary hydrogen bonds with main-chain atoms is smaller than the average B-factor of water molecules involved in secondary hydrogen bonds to protein atoms that form concurrent intramolecular hydrogen bonds. To study the structural coupling between internal waters and buried polar atoms in detail we simulated the dynamics of wild-type FKBP12, in which a buried water, Wat137, forms one side-chain and multiple main-chain hydrogen bonds. We mutated E60, whose side-chain hydrogen bonds with Wat137, to Q, N, S or A, to modulate the multiplicity and geometry of hydrogen bonds to the water. Mutating E60 to a residue that is unable to form a hydrogen bond with Wat137 results in reorientation of the water molecule and leads to a structural readjustment of residues that are both near and distant to the water. We predict that the E60A mutation will result in a significantly reduced affinity of FKBP12 for its ligand FK506. The propensity of internal waters to hydrogen bond to buried polar atoms suggests that ordered water molecules may constitute fundamental structural components of proteins, particularly in regions where alpha-helical or beta-sheet secondary structure is not present.     

Direct detection of hydrogen bonds in monomeric superoxide dismutase: biological implications

Hydrogen bonds were directly determined via NMR with different experimental approaches at 600 and 800 MHz for reduced monomeric superoxide dismutase (Q133M2SOD, 16 kDa). This protein contains a copper and a zinc ion and shows the classical superoxide dismutase (SOD) eight-stranded beta-barrel fold. The best results for this intermediate molecular mass protein were obtained using a TROSY version of the long-range HNCO experiment at high magnetic field (800 MHz) or with a cryoprobe at 600 MHz. The backbone hydrogen bond network that defines the secondary structure of the protein was detected. Thirty-five backbone hydrogen bonds were identified. The lower limit for their detection, their relation to the TROSY R(2) rates, and the correlation between hydrogen bond detectability and signal line width are discussed. Experiments were also optimized to detect hydrogen bonds involving key side chains, which lead to the observation of five hydrogen bonds. In particular, the hydrogen bonds involving the side chain of Asp 124 were observed, which show significant differences with respect to the bonds expected on the basis of the crystal structure. The relevance of this finding relies also on the fact that Asp 124 is a key residue in determining the affinity of the protein for zinc. It has now been determined that the gain of the toxic function of peroxynitrite formation in SOD mutants related to amyotrophic lateral sclerosis (ALS) is due to SOD species lacking the zinc ion, as a consequence of a reduced affinity for zinc. Therefore, this study provides structural hints for understanding the origin of the enzymatic behavior of the Zn-deficient SOD.     

Energy of hydrogen bonds probed by the adhesion of functionalized lipid layers

It is now well admitted that hydrophobic interactions and hydrogen bonds are the main forces driving protein folding and stability. However, because of the complex structure of a protein, it is still difficult to separate the different energetic contributions and have a reliable estimate of the hydrogen bond part. This energy can be quantified on simpler systems such as surfaces bearing hydrogen-bonding groups. Using the surface force apparatus, we have directly measured the interaction energy between monolayers of lipids whose headgroups can establish hydrogen bonds in water: nitrilotriacetate, adenosine, thymidine, and methylated thymidine lipids. From the adhesion energy between the surfaces, we have deduced the energy of a single hydrogen bond in water. We found in each case an energy of 0.5 kcal/mol. This result is in good agreement with recent experimental and theoretical studies made on protein systems showing that intramolecular hydrogen bonds make a positive contribution to protein stabilization.     

3 Nsec molecular dynamics simulation of the protein ubiquitin and comparison with X-ray crystal and solution NMR structures.

Mainly due to computational limitations, past protein molecular dynamics simulations have rarely been extended to 300 psec; we are not aware of any published results beyond 350 psec. The present work compares a 3000 psec simulation of the protein ubiquitin with the available x-ray crystallographic and solution NMR structures. Aside from experimental structure availability, ubiquitin was studied because of its relatively small size (76 amino acids) and lack of disulfide bridges. An implicit solvent model was used except for explicit treatment of waters of crystallization. We found that the simulated average structure retains most of the character of the starting x-ray crystal structure. In two highly surface accessible regions, the simulation was not in agreement with the x-ray structure. In addition, there are six backbone-backbone hydrogen bonds that are in conflict between the solution NMR and x-ray crystallographic structures; two are bonds that the NMR does not locate, and four are ones that the two methods disagree upon the donor. Concerning these six backbone-backbone hydrogen bonds, the present simulation agrees with the solution NMR structure in five out-of-the six cases, in that if a hydrogen bond is present in the x-ray structure and not in the NMR structure, the bond breaks within 700 psec. Of the two hydrogen bonds that are found in the NMR structure and not in the x-ray structure, one forms at 1400 psec and the other forms rarely. The present results suggest that relatively long molecular dynamics simulations, that use protein x-ray crystal coordinates for the starting structure and a computationally efficient solvent representation, may be used to gain an understanding of conformational and dynamic differences between the solid-crystal and dilute-solution states.     

Effects of ethanol on the secondary structure specific hydration properties of Chymotrypsin Inhibitor 2 in its folded and unfolded forms

Molecular dynamics simulations were performed for the protein Chymotrypsin Inhibitor 2 in water–ethanol binary mixtures at several ethanol concentrations at two different temperatures to explore the differential role of ethanol on the hydration properties of the secondary structural segments of the protein. We find that, compared to the water structure around the secondary structure segments of the unfolded protein in pure water, water molecules preferred to be structured more in presence of ethanol. The structuration of ethanol is noticed to be higher around helix and sheet, as compared to that around the loop. The differential slow structural relaxations of the hydrogen bonds involving the secondary structural segments of protein in water–ethanol mixed solutions, as compared to that in pure water infer that ethanol alters the water properties in a remarkable manner. The slow relaxations of the hydrogen bonds formed between ethanol and the secondary structural segments of the protein, in general, suggests that ethanol interacts directly with the protein. However, the relatively faster relaxation of the ethanol-segment hydrogen bonds involving unfolded protein as compared to that involving the folded protein suggests that the unfolded protein surface can remain dynamically free to interact with water more.     

Structural transformation of apocytochrome c induced by alternating copolymers of maleic acid and alkene

Apocytochrome c interacts with two copolymers: poly(isobutylene-alt-maleic acid) (PIMA) and poly(1-tetradecene-alt-maleic acid) (PTMA). The interaction leads to apocytochrome c, a conformational change from random coil to alpha-helical structure. The alpha-helix content is influenced by the copolymer concentration, the length of alkyl chain of the copolymers, and pH of the medium. The electrostatic attraction between the copolymer and protein is an indispensable factor for the folding of the protein at acid pH. The hydrophobic interaction is an important factor over the entire pH range, especially when both the copolymer and protein carry negative charges at alkaline pH. The electrostatic and hydrophobic attractions between the copolymer and protein exclude water molecules, promoting the formation of hydrogen bonds within the helical structure. On the other hand, the hydrogen bonds formed between the ionized carboxyl of the copolymer and the amide of the protein partly restrain the formation of hydrogen bonds within the helical structure when the copolymer concentration is higher at pH 6.5 and 10.5.     

High-resolution study of the three-dimensional structure of horse heart metmyoglobin

The three-dimensional structure of horse heart metmyoglobin has been refined to a final R-factor of 15.5% for all observed data in the 6.0 to 1.9 A resolution range. The final model consists of 1242 non-hydrogen protein atoms, 154 water molecules and one sulfate ion. This structure has nearly ideal bonding and bond angle geometry. A Luzzati plot of the variation in R-factor with resolution yields an estimated mean co-ordinate error of 0.18 A. An extensive analysis of the pattern of hydrogen bonds formed in horse heart metmyoglobin has been completed. Over 80% of the polypeptide chain is involved in eight helical segments, of which seven are composed mainly of alpha-helical (3.6(13))-type hydrogen bonds; the remaining helix is composed entirely of 3(10) hydrogen bonds. Altogether, of 102 hydrogen bonds between main-chain atoms only six are not involved in helical structures, and four of these six occur within beta-turns. The majority of water molecules in horse heart metmyoglobin are found in solvent networks that range in size from two to 35 members. The size of water molecule networks can be rationalized on the basis of three factors: the number of hydrogen bonds to the protein surface, the presence of charged side-chain atoms, and the ability to bridge to neighboring molecules in the crystal lattice. Bridging water networks form the dominant intermolecular interactions. The backbone conformation of horse heart metmyoglobin is very similar to sperm whale metmyoglobin, with significant differences in secondary structure occurring only near residues 119 and 120, where residues 120 to 123 in sperm whale form a distorted type I reverse turn and the horse heart protein has a type II turn at residues 119 to 122. Nearly all of the hydrogen bonds between main-chain atoms (occurring mainly in helical regions) are common to both proteins, and more than half of the hydrogen bonds involving side-chain atoms observed in horse heart are also found in sperm whale metmyoglobin. Unlike sperm whale metmyoglobin, the heme iron atom in horse heart metmyoglobin is not significantly displaced from the plane of the heme group.     

C-H...O hydrogen bonds in the nuclear receptor RARgamma--a potential tool for drug selectivity

Hydrogen bonds between polarized atoms play a crucial role in protein interactions and are often used in drug design, which usually neglects the potential of C-H...O hydrogen bonds. The 1.4 A resolution crystal structure of the ligand binding domain of the retinoic acid receptor RARgamma complexed with the retinoid SR11254 reveals several types of C-H...O hydrogen bonds. A striking example is the hydroxyl group of the ligand that acts as an H bond donor and acceptor, leading to a synergy between classical and C-H...O hydrogen bonds. This interaction introduces both specificity and affinity within the hydrophobic ligand pocket. The similarity of intraprotein and protein-ligand C-H...O interactions suggests that such bonds should be considered in rational drug design approaches.     

Energetics of protein folding

The energetics of protein folding determine the 3D structure of a folded protein. Knowledge of the energetics is needed to predict the 3D structure from the amino acid sequence or to modify the structure by protein engineering. Recent developments are discussed: major factors are reviewed and auxiliary factors are discussed briefly. Major factors include the hydrophobic factor (burial of non-polar surface area) and van der Waals interactions together with peptide hydrogen bonds and peptide solvation. The long-standing model for the hydrophobic factor (free energy change proportional to buried non-polar surface area) is contrasted with the packing-desolvation model and the approximate nature of the proportionality between free energy and apolar surface area is discussed. Recent energetic studies of forming peptide hydrogen bonds (gas phase) are reviewed together with studies of peptide solvation in solution. Closer agreement is achieved between the 1995 values for protein unfolding enthalpies in vacuum given by Lazaridis-Archontis-Karplus and Makhatadze-Privalov when the solvation enthalpy of the peptide group is taken from electrostatic calculations. Auxiliary factors in folding energetics include salt bridges and side-chain hydrogen bonds, disulfide bridges, and propensities to form alpha-helices and beta-structure. Backbone conformational entropy is a major energetic factor which is discussed only briefly for lack of knowledge.     

Structural evidence for guanidine-protein side chain interactions: crystal structure of CutA from Pyrococcus horikoshii in 3 M guanidine hydrochloride

This study was carried out to investigate the structural perturbation of the protein's local structure by the denaturants under non-denaturing conditions. Crystal structure of CutA from an archaeon Pyrococcus horikosii (PhoCutA), a heavy-metal binding protein, was determined at 1.6-angstroms resolution in the presence of 3 M guanidine HCl (GdnHCl). Native PhoCutA has a large number of short intramolecular hydrogen bonds and salt bridges on the protein surface, of which greater than 90% of hydrogen bonds and all salt bridges were retained in 3 M GdnHCl. Hydrogen bonds that disappeared in the GdnHCl crystal structure were mainly located on the protein surface, especially around the structurally perturbed loop, suggesting interactions between peptide groups and GdnHCl. Only a few GdnH+ ions were observed in the crystal structure, although none at the surface, of the protein. Two GdnH+ ions were observed in the center of the trimeric structure, replacing water molecules, and were hydrogen bonded with Asp84 and Asp86 of each chain. The exterior loop from Tyr39 to Lys44, including Trp40-Trp41, was perturbed structurally. Decreases in temperature factors were observed in beta strand 5 and the N terminus of helix 3. These results suggest the specific bindings of GdnH+ with some acidic residues and the non-specific bindings around Trp residues and peptide groups on the protein surface and that binding of GdnHCl to the native protein is limited, resulting in local structural perturbation.     

Deterministic features of side-chain main-chain hydrogen bonds in globular protein structures

A total of 19 835 polar residues from a data set of 250 non-homologous and highly resolved protein crystal structures were used to identify side-chain main-chain (SC-MC) hydrogen bonds. The ratio of the number of SC-MC hydrogen bonds to the total number of polar residues is close to 1:2, indicating the ubiquitous nature of such hydrogen bonds. Close to 56% of the SC-MC hydrogen bonds are local involving side-chain acceptor/donor ('i') and a main-chain donor/acceptor within the window i-5 to i+5. These short-range hydrogen bonds form well defined conformational motifs characterized by specific combinations of backbone and side-chain torsion angles. (a) The Ser/Thr residues show the greatest preference in forming intra-helical hydrogen bonds between the atoms O(gamma)(i) and O(i-4). More than half the examples of such hydrogen bonds are found at the middle of alpha-helices rather than at their ends. The most favoured motif of these examples is alpha(R)alpha(R)alpha(R)alpha(R)(g(-)). (b) These residues also show great preference to form hydrogen bonds between O(gamma)(i) and O(i-3), which are closely related to the previous type and though intra-helical, these hydrogen bonds are more often found at the C-termini of helices than at the middle. The motif represented by alpha(R)alpha(R)alpha(R)alpha(R)(g(+)) is most preferred in these cases. (c) The Ser, Thr and Glu are the most frequently found residues participating in intra-residue hydrogen bonds (between the side-chain and main-chain of the same residue) which are characterized by specific motifs of the form beta(g(+)) for Ser/Thr residues and alpha(R)(g(-)g(+)t) for Glu/Gln. (d) The side-chain acceptor atoms of Asn/Asp and Ser/Thr residues show high preference to form hydrogen bonds with acceptors two residues ahead in the chain, which are characterized by the motifs beta (tt')alphaR and beta(t)alpha(R), respectively. These hydrogen bonded segments, referred to as Asx turns, are known to provide stability to type I and type I' beta-turns. (e) Ser/Thr residues often form a combination of SC-MC hydrogen bonds, with the side-chain donor hydrogen bonded to the carbonyl oxygen of its own peptide backbone and the side-chain acceptor hydrogen bonded to an amide hydrogen three residues ahead in the sequence. Such motifs are quite often seen at the beginning of alpha-helices, which are characterized by the beta(g(+))alpha(R)alpha(R) motif. A remarkable majority of all these hydrogen bonds are buried from the protein surface, away from the surrounding solvent. This strongly indicates the possibility of side-chains playing the role of the backbone, in the protein interiors, to satisfy the potential hydrogen bonding sites and maintaining the network of hydrogen bonds which is crucial to the structure of the protein.     

Membrane protein folding: how important are hydrogen bonds?

Water is an inhospitable environment for protein hydrogen bonds because it is polarizable and capable of forming competitive hydrogen bonds. In contrast, the apolar core of a biological membrane seems like an ideal environment for hydrogen bonds, and it has long been assumed that hydrogen bonding should be a powerful force driving membrane protein folding. Nevertheless, while backbone hydrogen bonds may be much stronger in membrane proteins, experimental measurements indicate that side chain hydrogen bond strengths are not strikingly different in membrane and water soluble proteins. How is this possible? I argue that model compounds in apolar solvents do not adequately describe the system because the protein itself is ignored. The protein chain provides a rich source of competitive hydrogen bonds and a polarizable environment that can weaken hydrogen bonds. Thus, just like water soluble proteins, evolution can drive the creation of potent hydrogen bonds in membrane proteins where necessary, but mitigating forces in their environment must still be overcome.     

Mapping the lifetimes of local opening events in a native state protein.

The rate constants for the processes that lead to local opening and closing of the structures around hydrogen bonds in native proteins have been determined for most of the secondary structure hydrogen bonds in the four-helix protein acyl coenzyme A binding protein. In an analysis that combines these results with the energies of activation of the opening processes and the stability of the local structures, three groups of residues in the protein structure have been identified. In one group, the structures around the hydrogen bonds have frequent openings, every 600 to 1,500 s, and long lifetimes in the open state, around 1 s. In another group of local structures, the local opening is a very rare event that takes place only every 15 to 60 h. For these the lifetime in the open state is also around 1 s. The majority of local structures have lifetimes between 2,000 and 20,000 s and relatively short lifetimes of the open state in the range between 30 and 400 ms. Mapping of these groups of amides to the tertiary structure shows that the openings of the local structures are not cooperative at native conditions, and they rarely if ever lead to global unfolding. The results suggest a mechanism of hydrogen exchange by progressive local openings.