Partially unfolded equilibrium state of hen lysozyme studied by circular dichroism spectroscopy

Equilibrium unfolding of hen egg white lysozyme as a function of GdnCl concentration at pH 0.9 was studied over a temperature range 268.2-303.2 K by means of CD spectroscopy. As monitored by far- and near-UV CD at 222 and 289 nm, the lack of coincidence between two unfolding transition curves was observed, which suggests the existence of a third conformational species in addition to native and unfolded states. The three-state model, in which a stable intermediate is populated, was employed to estimate the thermodynamic parameters for the GdnCl-induced unfolding. It was found that the transition from the native to intermediate states proceeds with significant changes in enthalpy and entropy due to an extremely cooperative process, while the transition from the intermediate to unfolded states shows a low cooperativity with small enthalpy and entropy changes. These results indicate that the highest energy barrier for the GdnCl-induced unfolding of hen lysozyme is located in the process from the native state to the intermediate state, and this process is largely responsible for the cooperativity of protein unfolding.     

Salt bridge as a gatekeeper against partial unfolding

Salt bridges are frequently observed in protein structures. Because the energetic contribution of salt bridges is strongly dependent on the environmental context, salt bridges are believed to contribute to the structural specificity rather than the stability. To test the role of salt bridges in enhancing structural specificity, we investigated the contribution of a salt bridge to the energetics of native‐state partial unfolding in a cysteine‐free version of Escherichia coli ribonuclease H (RNase H*). Thermolysin cleaves a protruding loop of RNase H^* through transient partial unfolding under native conditions. Lys86 and Asp108 in RNase H^* form a partially buried salt bridge that tethers the protruding loop. Investigation of the global stability of K86Q/D108N RNase H^* showed that the salt bridge does not significantly contribute to the global stability. However, K86Q/D108N RNase H^* is greatly more susceptible to proteolysis by thermolysin than wild‐type RNase H^* is. The free energy for partial unfolding determined by native‐state proteolysis indicates that the salt bridge significantly increases the energy for partial unfolding by destabilizing the partially unfolded form. Double mutant cycles with single and double mutations of the salt bridge suggest that the partially unfolded form is destabilized due to a significant decrease in the interaction energy between Lys86 and Asp108 upon partial unfolding. This study demonstrates that, even in the case that a salt bridge does not contribute to the global stability, the salt bridge may function as a gatekeeper against partial unfolding that disturbs the optimal geometry of the salt bridge.     

pH-induced denaturation of proteins: a single salt bridge contributes 3-5 kcal/mol to the free energy of folding of T4 lysozyme

The energetics of a salt bridge formed between the side chains of aspartic acid 70 (Asp70) and histidine 31 (His31) of T4 lysozyme have been examined by nuclear magnetic resonance techniques. The pKa values of the residues in the native state are perturbed from their values in the unfolded protein such that His31 has a pKa value of 9.1 in the native state and 6.8 in the unfolded state at 10 degrees C in moderate salt. Similarly, the aspartate pKa is shifted to a value of about 0.5 in the native state from its value of 3.5-4.0 in the unfolded state. These shifts in pKa show that the salt bridge is stabilized 3-5 kcal/mol. This implies that the salt bridge stabilizes the native state by 3-5 kcal/mol as compared to the unfolded state. This is reflected in the thermodynamic stability of mutants of the protein in which Asp70, His31, or both are replaced by asparagine. These observations and consideration of the thermodynamic coupling of protonation state to folding of proteins suggest a mechanism of acid denaturation in which the unfolded state is progressively stabilized by protonation of its acid residues as pH is lowered below pH 4. The unfolded state is stabilized only if acidic groups in the folded state have lower pKa values than in the unfolded state. When the pH is sufficiently low, the acid groups of both the native and unfolded states are fully protonated, and the apparent unfolding equilibrium constant becomes pH independent. Similar arguments apply to base-induced unfolding.(ABSTRACT TRUNCATED AT 250 WORDS)     

Protein unfolding transitions in an intrinsically unstable annexin domain: molecular dynamics simulation and comparison with nuclear magnetic resonance data

Unfolding transitions of an intrinsically unstable annexin domain and the unfolded state structure have been examined using multiple approximately 10-ns molecular dynamics simulations. Three main basins are observed in the configurational space: native-like state, compact partially unfolded or intermediate compact state, and the unfolded state. In the native-like state fluctuations are observed that are nonproductive for unfolding. During these fluctuations, after an initial loss of approximately 20% of the core residue native contacts, the core of the protein transiently completely refolds to the native state. The transition from the native-like basin to the partially unfolded compact state involves approximately 75% loss of native contacts but little change in the radius of gyration or core hydration properties. The intermediate state adopts for part of the time in one of the trajectories a novel highly compact salt-bridge stabilized structure that can be identified as a conformational trap. The intermediate-to-unfolded state transition is characterized by a large increase in the radius of gyration. After an initial relaxation the unfolded state recovers a native-like topology of the domain. The simulated unfolded state ensemble reproduces in detail experimental nuclear magnetic resonance data and leads to a convincing complete picture of the unfolded domain.     

Energetics of three-state unfolding of a protein: canine milk lysozyme.

Thermodynamics of thermal transitions of a calcium-binding lysozyme, canine milk lysozyme (CML), was studied using differential scanning calorimetry and compared with those for homologous proteins, human alpha-lactalbumin (alpha-hLA) and equine milk lysozyme (EML). The results showed that CML and EML exhibit two clear heat absorption peaks in the absence of calcium ions (apo-form), although the cooperative thermal transition of alpha-hLA is apparently absent in this form. The first peak represents the unfolding transition from the native to an unfolding intermediate state (N-I transition) and the second peak represents that from the intermediate to the thermally unfolded state (I-U transition). We interpret that the cooperative thermal transition, which is observed between the intermediate and the thermally unfolded states of CML and EML, comes from the native-like packing interaction in their intermediate states. Furthermore, to examine the role of the stabilization mechanism of CML intermediate, we constructed four variant CMLs (H21G, I56L, A93S and V109K), in which the residues of CML are substituted for those of EML, and also investigated their thermal stability. Especially the His21 and Val109 of CML play a role in stabilization of the intermediate state and their contributions to the unfolding free energy are estimated to be 2.0 and 1.8 kJ/mol, respectively. From the results of the mutational analysis, a few differences in the local helical interactions within the alpha-domain are found to be predominant in stabilizing the intermediate state.     

Insights into conformation and dynamics of protein GB1 during folding and unfolding by NMR

Understanding protein stability requires characterization of structural determinants of the folded and unfolded states. Many proteins are capable of populating partially folded states under specific solution conditions. Occasionally, coexistence of the folded and an unfolded state under non- or mildly denaturing conditions can be observed by NMR, allowing us to structurally probe these states under identical conditions. Here we report on a destabilized mutant of the B1 domain of protein G (GB1) whose equilibrium unfolding was systematically investigated. Backbone amide residual dipolar couplings (RDCs), the tryptophan Nepsilon-H resonance and the amide nitrogen transverse relaxation rates (R2s) for varying pH values and different temperatures were measured. The backbone amide RDCs indicate that prior to complete unfolding, two melting hot spots are formed at the turn around T11, L12 and K13 and the N terminus of the helix at A24 and T25. The RDCs for the low pH, thermally unfolded state of GB1 are very small and do not indicate the presence of any native-like structure. Amide nitrogen transverse relaxation rates for GB1 in the folded state at different temperatures exhibit large contributions from exchange processes and the associated dynamics display considerable heterogeneity. Our data provide clear evidence for intermediate conformations and multi-state equilibrium un/folding for this GB1 variant.     

Cold denaturation of alpha-lactalbumin

We have investigated the thermal unfolding of bovine alpha-lactalbumin by means of circular dichroism spectroscopy in the far- and near-ultraviolet regions, and shown that the native alpha-lactalbumin undergoes heat and cold denaturation. The guanidine hydrochloride-induced unfolding of alpha-lactalbumin was also investigated by circular dichroism spectroscopy at various temperatures from 261 to 318 K. It is shown that the population of the molten globule state is strongly dependent on temperature and that the molten globule state does not accumulate during the guanidine hydrochloride-induced unfolding transition at 261 K. Our results indicate that the molten globule state of alpha-lactalbumin undergoes cold denaturation as the native alpha-lactalbumin does, and that the heat capacity change of unfolding from the molten globule to the unfolded state is positive and significant. The present results further support the idea that the molten globule and the unfolded states do not belong to the same thermodynamic state, and that the native, molten globule and unfolded states are sufficient for interpreting the guanidine hydrochloride-induced unfolding behavior of alpha-lactalbumin.     

Microsecond folding of the cold shock protein measured by a pressure-jump technique

A pressure-jump apparatus was employed in investigating the kinetics of protein unfolding and refolding. In the reaction cell, the pressure can be increased or decreased by 100-160 bar within 50-100 microseconds and then held constant. Thus, unfolding and refolding reactions in the time range from 70 microseconds to 70 s can be followed with this technique. Measurements are possible in the transition regions of thermally or denaturant-induced folding in a wide range of temperatures and solvent conditions. We used this pressure-jump method to determine the temperature dependence of the rate constants of unfolding and refolding of the cold shock protein of Bacillus subtilis and of three variants thereof with Phe --> Ala substitutions in the central beta-sheet region. For all variants, the change in heat capacity occurred in refolding between the unfolded and activated states, suggesting that the overall native-like character of the activated state of folding was not changed by the deletion of individual Phe side chains. The Phe27Ala mutation affected the rate of unfolding only; the Phe15Ala and Phe17Ala mutations changed the kinetics of both unfolding and refolding. Although the activated state of folding of the cold shock protein is overall native-like, individual side chains are still in a non-native environment.     

Diffusing and colliding: the atomic level folding/unfolding pathway of a small helical protein

Proteins with ultra-fast folding/unfolding kinetics are excellent candidates for study by molecular dynamics. Here, we describe such simulations of a three helix bundle protein, the engrailed homeodomain (En-HD), which folds via the diffusion-collision model. The unfolding pathway of En-HD was characterized by seven simulations of the protein and 12 simulations of its helical fragments yielding over 1.1 micros of simulation time in water. Various conformational states along the unfolding pathway were identified. There is the compact native-like transition state, a U-shaped helical intermediate and an unfolded state with dynamic helical segments. Each of these states is in good agreement with experimental data. Examining these states as well as the transitions between them, we find the role of long-range tertiary contacts, specifically salt-bridges, important in the folding/unfolding pathway. In the folding direction, charged residues form long-range tertiary contacts before the hydrophobic core is formed. The formation of HII is assisted by a specific salt-bridge and by non-specific (fluctuating) tertiary contacts, which we call contact-assisted helix formation. Salt-bridges persist as the protein approaches the transition state, stabilizing HII until the hydrophobic core is formed. To complement this information, simulations of fragments of En-HD illustrate the helical propensities of the individual segments. By thermal denaturation, HII proved to be the least stable helix, unfolding in less than 450 ps at high temperature. We observed the low helical propensity of C-terminal residues from HIII in fragment simulations which, when compared to En-HD unfolding simulations, link the unraveling of HIII to the initial event that drives the unfolding of En-HD.     

Unfolding of a Small Protein Proceeds via Dry and Wet Globules and a Solvated Transition State

Dissecting a protein unfolding process into individual steps can provide valuable information on the forces that maintain the integrity of the folded structure. Solvation of the protein core determines stability, but it is not clear when such solvation occurs during unfolding. In this study, far-UV circular dichroism measurements suggest a simplistic two-state view of the unfolding of barstar, but the use of multiple other probes brings out the complexity of the unfolding reaction. Near-UV circular dichroism measurements show that unfolding commences with the loosening of tertiary interactions in a native-like intermediate, N^∗. Fluorescence resonance energy transfer measurements show that N^∗ then expands rapidly but partially to form an early unfolding intermediate I_E. Fluorescence spectral measurements indicate that both N^∗ and I_E have retained native-like solvent accessibility of the core, suggesting that they are dry molten globules. Dynamic quenching measurements at the single tryptophan buried in the core suggest that the core becomes solvated only later in a late wet molten globule, I_L, which precedes the unfolded form. Fluorescence anisotropy decay measurements show that tight packing around the core tryptophan is lost when I_L forms. Of importance, the slowest step is unfolding of the wet molten globule and involves a solvated transition state.     

Unfolding of a Small Protein Proceeds via Dry and Wet Globules and a Solvated Transition State

Dissecting a protein unfolding process into individual steps can provide valuable information on the forces that maintain the integrity of the folded structure. Solvation of the protein core determines stability, but it is not clear when such solvation occurs during unfolding. In this study, far-UV circular dichroism measurements suggest a simplistic two-state view of the unfolding of barstar, but the use of multiple other probes brings out the complexity of the unfolding reaction. Near-UV circular dichroism measurements show that unfolding commences with the loosening of tertiary interactions in a native-like intermediate, N^∗. Fluorescence resonance energy transfer measurements show that N^∗ then expands rapidly but partially to form an early unfolding intermediate I_E. Fluorescence spectral measurements indicate that both N^∗ and I_E have retained native-like solvent accessibility of the core, suggesting that they are dry molten globules. Dynamic quenching measurements at the single tryptophan buried in the core suggest that the core becomes solvated only later in a late wet molten globule, I_L, which precedes the unfolded form. Fluorescence anisotropy decay measurements show that tight packing around the core tryptophan is lost when I_L forms. Of importance, the slowest step is unfolding of the wet molten globule and involves a solvated transition state.     

Characterizing intermolecular interactions that initiate native-like protein aggregation

Folded proteins can access aggregation-prone states without the need for transitions that cross the energy barriers for unfolding. In this study we characterized the initial steps of aggregation from a native-like state of the acylphosphatase from Sulfolobus solfataricus (Sso AcP). Using computer simulations restrained by experimental hydrogen/deuterium (H/D) exchange data, we provide direct evidence that under aggregation-promoting conditions Sso AcP populates a conformational ensemble in which native-like structure is retained throughout the sequence in the absence of local unfolding (N¹), although the protein exhibits an increase in hydrodynamic radius and dynamics. This transition leads an edge strand to experience an increased affinity for a specific unfolded segment of the protein. Direct measurements by means of H/D exchange rates, isothermal titration calorimetry, and intermolecular relaxation enhancements show that after formation of N¹, an intermolecular interaction with an antiparallel arrangement is established between the edge strand and the unfolded segment of the protein. However, under conditions that favor the fully native state of Sso AcP, such an interaction is not established. Thus, these results reveal a novel (to our knowledge) self-assembly mechanism for a folded protein that is based on the increased flexibility of highly aggregation-prone segments in the absence of local unfolding.     

Calorimetric evidence for a native-like conformation of hen egg-white lysozyme dissolved in glycerol

Hen egg-white lysozyme, lyophilized from aqueous solutions of different pH (from pH 2.5 to 10.0) and then dissolved in water and in anhydrous glycerol, has been studied by high-sensitivity differential scanning microcalorimetry over the temperature range from 10 to 150 degrees C. All lysozyme samples exhibit a cooperative conformational transition in both solvents occurring between 10 and 100 degrees C. The transition temperatures in glycerol are similar to those in water at the corresponding pHs. The transition enthalpies in glycerol are substantially lower than in water but follow similar pH dependences. The transition heat capacity increment in glycerol does not depend on the pH and is 1.25+/-0.31 kJ mol(-1) K(-1), which is less than one fifth of that in water (6. 72+/-0.23 kJ mol(-1) K(-1)). The thermal transition in glycerol is reversible and equilibrium, as demonstrated for the pH 8.0 sample, and follows the classical two-state mechanism. In contrast to lysozyme in water, the protein dissolved in glycerol undergoes an additional, irreversible cooperative transition with a marginal endothermic heat effect at temperatures of 120-130 degrees C. The transition temperature of this second transition increases with the heating rate which is characteristic of kinetically controlled processes. Thermodynamic analysis of the calorimetric data reveals that the stability of the folded conformation of lysozyme in glycerol is similar to that in water at 20-80 degrees C but exceeds it at lower and higher temperatures. It is hypothesized that the thermal unfolding in glycerol follows the scheme: N ifho-MG-->U, where N is a native-like conformation, ho-MG is a highly ordered molten globule state, and U is the unfolded state of the protein.     

Snapshots of protein folding. A study on the multiple transition state pathway of cytochrome c(551) from Pseudomonas aeruginosa

Cytochrome c(551) (cyt c(551)) from Pseudomonas aeruginosa is a small protein (82 residues) that folds via a three-state pathway with the accumulation in the microsecond time-range of a compact collapsed intermediate. The presence of a single His residue, at position 16, permits the study of the refolding at pH 7.0 in the absence of miscoordination events. Here, we report on folding kinetics in the millisecond time-range as a function of urea under different pH conditions. Analysis of this process (over-and-above proline cis-trans isomerization) at pH 7.0, suggests the existence of a multiple transition state pathway in which we postulate three transition states. Taking advantage of site-directed mutagenesis we propose that the first "unfolded-like" transition state (t(1)) originates from the electrostatic properties of the collapsed state, while the second transition state (t(2)) involves the interaction between the N and C-terminal helices and is stabilized by the salt bridge between Lys10 and Glu70 ( approximately 1 kcal mol(-1)). Our results suggest that, contrary to other cytochromes c, the roll-over effect observed for cyt c(551) at low denaturant concentration can be interpreted in terms of a broad energy barrier without population of any intermediates. The third and more "native-like" transition state (M) can be associated with the breaking/formation of the Fe(3+)-Met61 bond. This strong interaction is stabilized by the hydrogen bond between Trp56 and heme propionate 17 (HP-17) as suggested by the increase in the unfolding rate at high denaturant concentration of the Trp56Phe site-directed mutant.     

Increasing temperature accelerates protein unfolding without changing the pathway of unfolding

We have traditionally relied on extremely elevated temperatures (498K, 225 degrees C) to investigate the unfolding process of proteins within the timescale available to molecular dynamics simulations with explicit solvent. However, recent advances in computer hardware have allowed us to extend our thermal denaturation studies to much lower temperatures. Here we describe the results of simulations of chymotrypsin inhibitor 2 at seven temperatures, ranging from 298K to 498K. The simulation lengths vary from 94ns to 20ns, for a total simulation time of 344ns, or 0.34 micros. At 298K, the protein is very stable over the full 50ns simulation. At 348K, corresponding to the experimentally observed melting temperature of CI2, the protein unfolds over the first 25ns, explores partially unfolded conformations for 20ns, and then refolds over the last 35ns. Above its melting temperature, complete thermal denaturation occurs in an activated process. Early unfolding is characterized by sliding or breathing motions in the protein core, leading to an unfolding transition state with a weakened core and some loss of secondary structure. After the unfolding transition, the core contacts are rapidly lost as the protein passes on to the fully denatured ensemble. While the overall character and order of events in the unfolding process are well conserved across temperatures, there are substantial differences in the timescales over which these events take place. We conclude that 498K simulations are suitable for elucidating the details of protein unfolding at a minimum of computational expense.     

Alkaline unfolding and salt-induced folding of arginine kinase from shrimp Feneropenaeus chinensis under high pH conditions

The structural and functional properties of arginine kinase (AK) in alkaline conditions in the absence or presence of salt have been investigated. The conformational changes of AK during alkaline unfolding and salt-induced folding at alkaline pH were monitored using intrinsic fluorescence emission, binding of the fluorescence probe 1-anilino-8-naphthalenesulfonate and circular dichroism. The results for the alkaline unfolded enzyme showed that much lower pH (11.0) was required to cause the complete loss of AK activity than was required to cause an obvious conformational change of the enzyme. Compared with the completely unfolded state in 5 M urea, the high pH denatured enzyme had some residual secondary and tertiary structure even at pH 13.0. Increasing the ionic strength by adding salt at pH 12.75 resulted in the formation of a relatively compact tertiary structure and a little new secondary structure with hydrophobic surface enhancement. These results indicate that the partially folded state formed under alkaline conditions may have similarities to the molten globule state which is compact, but it has a poorly defined tertiary structure and a native-like secondary structure.     

Identification of equilibrium and kinetic intermediates involved in folding of urea-denatured creatine kinase

The unfolding transition and kinetic refolding of dimeric creatine kinase after urea denaturation were monitored by intrinsic fluorescence and far ultraviolet circular dichroism. An equilibrium intermediate and a kinetic folding intermediate were identified and characterized. The fluorescence intensity of the equilibrium intermediate is close to that of the unfolded state, whereas its ellipticity at 222 nm is about 50% of the native state. The transition curves measured by these two methods are therefore non-coincident. The kinetic folding intermediate, formed during the burst phase of refolding under native-like conditions, possesses 75% of the native secondary structure, but is mostly lacking in native tertiary structure. In moderate concentrations of urea, only the initial, rapid change in fluorescence intensity or negative ellipticity is observed, and the final state values do not reach the equivalent unfolding values. The unfolding and refolding transition curves measured under identical conditions are non-coincident within the transition from intermediate to fully unfolded state. It is observed by SDS-PAGE that disulfide bond-linked dimeric or oligomeric intermediates are formed in moderate urea concentrations, especially in the refolding reaction. These rapidly formed, soluble intermediates represent an off-pathway event that leads to the hysteresis in the refolding transition curves.     

Unfolding of the cold shock protein studied with biased molecular dynamics

The cold shock protein from Bacillus caldolyticus is a small beta-barrel protein that folds in a two-state mechanism. For the native protein and for several mutants, a wealth of experimental data are available on stability and folding, so that it is an optimal system to study this process. We compare data from unfolding simulations (trajectories of 5 and up to 12 ns) obtained with a bias potential at room temperature and from unbiased thermal unfolding simulations with experimental data. The unfolding patterns derived from the trajectories starting from different native-like conformations and subject to different unfolding conditions agree. The transition state found in the simulations of unfolding is close to the native structure in agreement with experiment. Moreover, a lower value of the free energy barrier of unfolding was found for the mutant R3E than for the mutant E46A and the native protein, as indicated by experimental data. The first unfolding event involves the three-stranded beta-sheet whose decomposition corresponds to the transition state. In contrast to conclusions drawn from experiments, we found that the two-stranded beta-strand forms the most stable substructure, which decomposes very late in the unfolding process. However, assuming that this structure forms very early in the folding process, our findings would not contradict the experiments but require a different interpretation of them.     

Microscopic reversibility of protein folding in molecular dynamics simulations of the engrailed homeodomain

The principle of microscopic reversibility states that at equilibrium the number of molecules entering a state by a given path must equal those exiting the state via the same path under identical conditions or, in structural terms, that the conformations along the two pathways are the same. There has been some indirect evidence indicating that protein folding is such a process, but there have been few conclusive findings. In this study, we performed molecular dynamics simulations of an ultrafast unfolding and folding protein at its melting temperature to observe, on an atom-by-atom basis, the pathways the protein followed as it unfolded and folded within a continuous trajectory. In a total of 0.67 micros of simulation in water, we found six transient denaturing events near the melting temperature (323 and 330 K) and an additional refolding event following a previously identified unfolding event at a high temperature (373 K). In each case, unfolding and refolding transition state ensembles were identified, and they agreed well with experiment on the basis of a comparison of S and Phi values. On the basis of several structural properties, these 13 transition state ensembles agreed very well with each other and with four previously identified transition states from high-temperature denaturing simulations. Thus, not only were the unfolding and refolding transition states part of the same ensemble, but in five of the seven cases, the pathway the protein took as it unfolded was nearly identical to the subsequent refolding pathway. These events provide compelling evidence that protein folding is a microscopically reversible process. In the other two cases, the folding and unfolding transition states were remarkably similar to each other but the paths deviated.     

Conformational restrictions on the pathway of folding and unfolding of the pancreatic trypsin inhibitor

The kinetic roles of the partially folded, intermediate protein species with two disulphide bonds in folding and unfolding of the pancreatic trypsin inhibitor have been investigated further. Formation of a second disulphide bond between Cys5 and Cys55 during refolding of the reduced inhibitor, which would yield the species with the 30–51 and 5–55 disulphide bonds and, possibly, the native-like conformation of the protein, is not significant. Instead, three other second disulphide bonds (5–14, 5–38 and 14–38) are formed approximately 10⁵ times more readily, but each of these two-disulphide species then rearranges intramolecularly to the native-like, two-disulphide intermediate. Therefore, the reduced protein does not simply form sequentially the three disulphide bonds of the native state. Unfolding of the native state takes place by the reverse of this process.The kinetic importance for folding and unfolding of this transition between two-disulphide intermediates under the conditions used here was illustrated experimentally by a modified form of the inhibitor in which the thiols of Cys14 and Cys38 were blocked irreversibly. In the folded conformation, this modified protein is more stable to unfolding than normal, but after unfolding cannot readily regain the native-like conformation, because Cys14 or Cys38 are required to be involved in disulphide bonds during the interconversion of the two-disulphide intermediates.Some conception of the conformational transitions that take place at each stage of the folding transition may be inferred from the relative propensities of the six cysteine residues to make or rearrange disulphide bonds. It is concluded that the inhibitor probably does not refold by sequential adoption of the native conformation by the unfolded polypeptide chain. Instead, it appears that essentially all elements of the native conformation are attained simultaneously in the final stage of folding, within an unstable and flexible, yet relatively compact, form of the entire polypeptide chain produced by weak interactions between groups distant in the primary structure.