EX1 hydrogen exchange and protein folding

Slow amide hydrogen exchange is an increasingly popular tool for investigating structure and function in proteins. The kinetic model for slow hydrogen exchange has two limits, called EX2 and EX1, wherein the thermodynamics and kinetics of protein motions, respectively, are reported by the exchange data. While many laboratories have demonstrated that EX2 exchange can indeed provide accurate results regarding the thermodynamics of protein stability, the potential of EX1 exchange to follow the kinetics of protein unfolding and folding is only beginning to be realized. EX1 hydrogen exchange has advantages over more traditional folding experiments: it provides single-residue resolution, as well as whole-molecule information, the latter of which can be interpreted in terms of the cooperativity of unfolding. However, key questions remain regarding the interpretation of EX1 hydrogen exchange.     

Beyond the EX1 limit: probing the structure of high-energy states in protein unfolding

Hydrogen exchange kinetics in native solvent conditions have been used to explore the conformational fluctuations of an immunoglobulin domain (CD2.domain1). The global folding/unfolding kinetics of the protein are unaltered between pH 4.5 and pH 9.5, allowing us to use the pH-dependence of amide hydrogen/deuterium exchange to characterise conformational states with energies up to 7.2kcal/mol higher than the folded ground state. The study was intended to search for discreet unfolding intermediates in this region of the energy spectrum, their presence being revealed by the concerted exchange behaviour of subsets of amide groups that become accessible at a given free energy, i.e. the spectrum would contain discreet groupings. Protection factors for 58 amide groups were measured across the pH range and the hydrogen-exchange energy profile is described.More interestingly, exchange behaviour could be grouped into three categories; the first two unremarkable, the third unexpected. (1) In 33 cases, amide exchange was dominated by rapid fluctuation, i.e. the free energy difference between the ground state and the rapidly accessed open state is sufficiently low that the contribution from crossing the unfolding barrier is negligible. (2) In 18 cases exchange is dominated by the global folding transition barrier across the whole pH range measured. The relationship between hydroxyl ion concentration and observed exchange rate is hyperbolic, with the limiting rate being that for global unfolding; the so-called EX1 limit. For these, the free energy difference between the folded ground state and any rapidly-accessed open state is too great for the proton to be exchanged through such fluctuations, even at the highest pH employed in this study. (3) For the third group, comprising five cases, we observe a behaviour that has not been described. In this group, as in category 2, the rate of exchange reaches a plateau; the EX1 limit. However, as the intrinsic exchange rate (k(int)) is increased, this limit is breached and the rate begins to rise again. This unintuitive behaviour does not result from pH instability, rather it is a consequence of amide groups experiencing two processes; rapid fluctuation of structure and crossing the global barrier for unfolding. The boundary at which the EX1 limit is overcome is determined by the equilibrium distribution of the fluctuating open and closed states (K(O/C)) and the rate constant for unfolding (k(u)). This critical boundary is reached when k(int)K(O/C)=k(u). Given that, in a simple transition state formalism: k(u)=K(#)k' (where K(#) describes the equilibrium distribution between the transition and ground state and k' describes the rate of a barrierless rearrangement), it follows that if the pH is raised to a level where k(int)=k', then the entire free energy spectrum from ground state to transition state could be sampled.     

Stability and folding properties of a model beta-sheet protein, Escherichia coli CspA.

Although beta-sheets represent a sizable fraction of the secondary structure found in proteins, the forces guiding the formation of beta-sheets are still not well understood. Here we examine the folding of a small, all beta-sheet protein, the E. coli major cold shock protein CspA, using both equilibrium and kinetic methods. The equilibrium denaturation of CspA is reversible and displays a single transition between folded and unfolded states. The kinetic traces of the unfolding and refolding of CspA studied by stopped-flow fluorescence spectroscopy are monoexponential and thus also consistent with a two-state model. In the absence of denaturant, CspA refolds very fast with a time constant of 5 ms. The unfolding of CspA is also rapid, and at urea concentrations above the denaturation midpoint, the rate of unfolding is largely independent of urea concentration. This suggests that the transition state ensemble more closely resembles the native state in terms of solvent accessibility than the denatured state. Based on the model of a compact transition state and on an unusual structural feature of CspA, a solvent-exposed cluster of aromatic side chains, we propose a novel folding mechanism for CspA. We have also investigated the possible complications that may arise from attaching polyhistidine affinity tags to the carboxy and amino termini of CspA.     

Role of a solvent-exposed aromatic cluster in the folding of Escherichia coli CspA

Escherichia coli CspA is a member of the cold shock protein family. All cold shock proteins studied to date fold rapidly by an apparent two-state mechanism. CspA contains an unusual cluster of aromatic amino acids on its surface that is necessary for nucleic acid binding and also provides stability to CspA (Hillier et al., 1998). To elucidate the role this aromatic cluster plays in the determining the folding rate and pathway of CspA, we have studied the folding kinetics of mutants containing either leucine or serine substituted for Phe 18, Phe20, and/or Phe31. The leucine substitutions are found to accelerate folding and the serine substitutions to decelerate folding. Because these residues exert effects on the free energy of the folding transition state, they may be necessary for nucleating folding. They are not responsible, however, for the very compact, native-like transition state ensemble seen in the cold shock proteins, as the refolding rates of the mutants all show a similar, weak dependence of unfolding rate on denaturant concentration. Using mutant cycle analysis, we show that there is energetic coupling among the three residues between the unfolded and transition states, suggesting that the cooperative nature of these interactions helps to determine the unfolding rate. Overall, our results suggest that separate evolutionary pressures can act simultaneously on the same group of residues to maintain function, stability, and folding rate.     

Partially folded states of staphylococcal nuclease highlight the conserved structural hierarchy of OB-fold proteins

We have been interested in whether three proteins that share a five-stranded beta-barrel "OB-fold" structural motif but no detectable sequence homology fold by similar mechanisms. Here we describe native-state hydrogen exchange experiments as a function of urea for SN (staphylococcal nuclease), a protein with an OB-fold motif and additional nonconserved elements of structure. The regions of structure with the largest stability and unfolding cooperativity are contained within the conserved OB-fold portion of SN, consistent with previous results for CspA (cold shock protein A) and LysN (anticodon binding domain of lysyl tRNA synthetase). The OB-fold also has the subset of residues with the slowest unfolding rates in the three proteins, as determined by hydrogen exchange experiments in the EX1 limit. Although the protein folding hierarchy is maintained at the level of supersecondary structure, it is not evident for individual residues as might be expected if folding depended on obligatory nucleation sites. Rather, the site-specific stability profiles appear to be linked to sequence hydrophobicity and to the density of long-range contacts at each site in the three-dimensional structures of the proteins. We discuss the implications of the correlation between stability to unfolding and conservation of structure for mechanisms of protein structure evolution.     

Examination of the folding of E. coli CspA through tryptophan substitutions

Escherichia coli cold shock protein, CspA, folds very rapidly (time constant, tau = 4 msec) by an apparent two-state mechanism. However, recent time-resolved infrared (IR) temperature-jump experiments indicate that the folding trajectory of CspA may be more complicated. The sole tryptophan of wild-type CspA (Trp11), which is used to monitor the folding process by fluorescence spectroscopy, is located in an unusual aromatic cluster on the surface of CspA within the nucleic acid binding site. To gain a more global picture of the folding kinetics of CspA and to determine if there are any previously undetected intermediates, we have introduced a second tryptophan at three different surface locations in the protein. The three mutations did not significantly alter the tertiary structure of CspA, although two of the substitutions were found to be slightly stabilizing. Two-state folding, as detected by stopped-flow fluorescence spectroscopy, is preserved in all three mutants. These results indicate that the fast folding of CspA is driven by a concerted mechanism.     

Microsecond to minute dynamics revealed by EX1-type hydrogen exchange at nearly every backbone hydrogen bond in a native protein

A previous comprehensive analysis of the pH dependence of native-state amide hydrogen (NH) exchange in turkey ovomucoid third domain (OMTKY3) yielded apparent opening and closing rate constants (k(op) and k(cl)) at 14 NH groups involved in global conformational changes. This analysis has been extended to 18 additional slowly exchanging NH groups. Quench-flow experiments were performed to monitor NH exchange in native OMTKY3 from neutral to very alkaline pH ( approximately 12) conditions. Above pH 10 the mechanism of exchange switched from one governed by a rapid equilibrium preceding the chemistry of exchange (i.e. EX2 exchange), to one where exchange was limited by the rate of opening (i.e. EX1 exchange). Kinetics of solvent exposure are now known for nearly all backbone NH groups in native OMTKY3, yielding rate constants that span five orders of magnitude, 0.004 to 200 s(-1).     

Contribution of proton linkage to the thermodynamic stability of the major cold-shock protein of Escherichia coli CspA

The stability of protein is defined not only by the hydrogen bonding, hydrophobic effect, van der Waals interactions, and salt bridges. Additional, much more subtle contributions to protein stability can arise from surface residues that change their properties upon unfolding. The recombinant major cold shock protein of Escherichia coli CspA an all-beta protein unfolds reversible in a two-state manner, and behaves in all other respects as typical globular protein. However, the enthalpy of CspA unfolding strongly depends on the pH and buffer composition. Detailed analysis of the unfolding enthalpies as a function of pH and buffers with different heats of ionization shows that CspA unfolding in the pH range 5.5-9.0 is linked to protonation of an amino group. This amino group appears to be the N-terminal alpha-amino group of the CspA molecule. It undergoes a 1.6 U shift in pKa values between native and unfolded states. Although this shift in pKa is expected to contribute approximately 5 kJ/mol to CspA stabilization energy the experimentally observed stabilization is only approximately 1 kJ/mol. This discrepancy is related to a strong enthalpy-entropy compensation due, most likely, to the differences in hydration of the protonated and deprotonated forms of the alpha-amino group.     

Equilibrium amide hydrogen exchange and protein folding kinetics

The classical Linderstrøm-Lang hydrogen exchange (HX) model is extended to describe the relationship between the HX behaviors (EX1 and EX2) and protein folding kinetics for the amide protons that can only exchange by global unfolding in a three-state system including native (N), intermediate (I), and unfolded (U) states. For these slowly exchanging amide protons, it is shown that the existence of an intermediate (I) has no effect on the HX behavior in an off-pathway three-state system (IUN). On the other hand, in an on-pathway three-state system (UIN), the existence of a stable folding intermediate has profound effect on the HX behavior. It is shown that fast refolding from the unfolded state to the stable intermediate state alone does not guarantee EX2 behavior. The rate of refolding from the intermediate state to the native state also plays a crucial role in determining whether EX1 or EX2 behavior should occur. This is mainly due to the fact that only amide protons in the native state are observed in the hydrogen exchange experiment. These new concepts suggest that caution needs to be taken if one tries to derive the kinetic events of protein folding from equilibrium hydrogen exchange experiments.     

Energetics of the native energy landscape of a two-domain calcium sensor protein: distinct folding features of the two domains

The protein folding energy landscape allows a thorough understanding of the protein folding problem which in turn helps in understanding various aspects of biological functions. Characterizing the cooperative unfolding units and the intermediates along the folding funnel of a protein is a challenging task. In this paper, we investigated the native energy landscape of EhCaBP, a calcium sensor, belonging to the same EF-hand superfamily as calmodulin. EhCaBP is a two-domain EF-hand protein consisting of two EF-hands in each domain and binding to four Ca2+ cations. Native-state hydrogen exchange (HX) was used to assess the folding features of the landscape and also to throw light on the structure-folding function paradigm of calcium sensor proteins. HX measurements under the EX2 regime provided the thermodynamic information about the protein folding events under native conditions. HX studies revealed that the unfolding of EhCaBP is not a two-state process. Instead, it proceeds through cooperative units. The C-terminal domain exhibits less denaturant dependence than the N-terminal domain, suggesting that the former is dominated by local fluctuations. It is interesting to note that the N- and C-terminal domains of EhCaBP have distinct folding features. In fact, these observed differences can regulate the domain-dependent target recognition of two-domain Ca2+ sensor proteins.     

Identification of rare partially unfolded states in equilibrium with the native conformation in an all beta-barrel protein

Human acidic fibroblast growth factor 1 (hFGF-1) is an all beta-barrel protein, and the secondary structural elements in the protein include 12 antiparallel beta-strands arranged into a beta-trefoil fold. In the present study, we investigate the stability of hFGF-1 by hydrogen-deuterium exchange as a function of urea concentration. Urea-induced equilibrium unfolding of hFGF-1 monitored by fluorescence and CD spectroscopy suggests that the protein unfolds by a two-state (native to denatured) mechanism. Hydrogen exchange in hFGF-1, under the experimental conditions used, occurs by the EX2 mechanism. In contrast to the equilibrium unfolding events monitored by optical probes, native state hydrogen exchange data show that the beta-trefoil architecture of hFGF-1 does not behave as a single cooperative unit. There are at least two structurally independent units with differing stabilities in hFGF-1. Beta-strands I, II, III, VI, VII, X, XI, and XII fit into the global unfolding isotherm. By contrast, residues in beta-strands IV, V, VIII, and IX exchange by the subfolding isotherm and could be responsible for the occurrence of high-energy partially unfolded state(s) in hFGF-1. There appears to be a broad continuum of stabilities among the four beta-strands (beta-strands IV, V, VIII, and IX) constituting the subglobal folding unit. The slow exchanging residues in hFGF-1 do not represent the folding nucleus of the protein.     

Intimate view of a kinetic protein folding intermediate: residue-resolved structure, interactions, stability, folding and unfolding rates, homogeneity

A cytochrome c kinetic folding intermediate was studied by hydrogen exchange (HX) pulse labeling. Advances in the technique and analysis made it possible to define the structured and unstructured regions, equilibrium stability, and kinetic opening and closing rates, all at an amino acid-resolved level. The entire N-terminal and C-terminal helices are formed and docked together at their normal native positions. They fray in both directions from the interaction region, due to a progression in both unfolding and refolding rates, leading to the surprising suggestion that helix propagation may proceed very slowly in the condensed milieu. Several native-like beta turns are formed. Some residues in the segment that will form the native 60s helix are protected but others are not, suggesting energy minimization to some locally non-native conformation in the transient intermediate. All other regions are unprotected, presumably dynamically disordered. The intermediate resembles a partially constructed native state. It is early, on-pathway, and all of the refolding molecules pass through it. These and related results consistently point to distinct, homogeneous, native-like intermediates in a stepwise sequential pathway, guided by the same factors that determine the native structure. Previous pulse labeling efforts have always assumed EX2 exchange during the labeling pulse, often leading to the suggestion of heterogeneous intermediates in alternative parallel pathways. The present work reveals a dominant role for EX1 exchange in the high pH labeling pulse, which will mimic heterogeneous behavior when EX2 exchange is assumed. The general problem of homogeneous versus heterogeneous intermediates and pathways is discussed.     

Equilibrium hydrogen exchange reveals extensive hydrogen bonded secondary structure in the on-pathway intermediate of Im7

The four-helical immunity protein Im7 folds through an on-pathway intermediate that has a specific, but partially misfolded, hydrophobic core. In order to gain further insight into the structure of this species, we have identified the backbone hydrogen bonds formed in the ensemble by measuring the amide exchange rates (under EX2 conditions) of the wild-type protein and a variant, I72V. In this mutant the intermediate is significantly destabilised relative to the unfolded state (deltadeltaG(ui) = 4.4 kJ/mol) but the native state is only slightly destabilised (deltadeltaG(nu) = 1.8 kJ/mol) at 10 degrees C in 2H2O, pH* 7.0 containing 0.4 M Na2SO4, consistent with the view that this residue forms significant non-native stabilising interactions in the intermediate state. Comparison of the hydrogen exchange rates of the two proteins, therefore, enables the state from which hydrogen exchange occurs to be identified. The data show that amides in helices I, II and IV in both proteins exchange slowly with a free energy similar to that associated with global unfolding, suggesting that these helices form highly protected hydrogen-bonded helical structure in the intermediate. By contrast, amides in helix III exchange rapidly in both proteins. Importantly, the rate of exchange of amides in helix III are slowed substantially in the Im7* variant, I72V, compared with the wild-type protein, whilst other amides exchange more rapidly in the mutant protein, in accord with the kinetics of folding/unfolding measured using chevron analysis. These data demonstrate, therefore, that local fluctuations do not dominate the exchange mechanism and confirm that helix III does not form stable secondary structure in the intermediate. By combining these results with previously obtained Phi-values, we show that the on-pathway folding intermediate of Im7 contains extensive, stable hydrogen-bonded structure in helices I, II and IV, and that this structure is stabilised by both native and non-native interactions involving amino acid side-chains in these helices.     

A kinetic folding intermediate probed by native state hydrogen exchange

Stopped-flow fluorescence studies on the N-terminal domain of rat CD2 (CD2.d1) have demonstrated that folding from the fully denatured state (U) proceeds via the transient accumulation of an apparent intermediate (I) in a so-called burst phase that precedes the rate-limiting transition leading to the native state (N). A previous pH-dependent equilibrium hydrogen exchange (HX) study identified a subset of amides in CD2.d1 which, under EX2 conditions, exchange from N with free energies greater than or equal to the free energy difference between the N and I states calculated from the stopped-flow data. Under EX1 conditions the rates of HX for these amides tend towards an asymptote that matches the global unfolding rate calculated from the stopped-flow data, suggesting that exchange for these amides requires traversing the N-to-I transition state barrier. Exchange for these amides presumably occurs from exchange-competent forms comprising the kinetic burst phase therefore. To explore this idea further, native state HX (NHX) data have been collected for CD2.d1 under EX2 conditions using denaturant concentrations which span either side of the denaturant concentration where, according to the stopped-flow data, the apparent U and I states are iso-energetic. The data fit to a two-component, sub-global (sg)/global (g) NHX mechanism, yielding Delta G and m value parameters (where the m value is a measure of hydrocarbon solvation). Regression analysis demonstrates that the (m(sg), Delta G(sg)) and (m(g), Delta G(g)) values calculated for this subset of amides correspond with those describing the kinetic burst phase transition. This result confirms the ability of the NHX technique to explore the structural and energetic properties of kinetic folding intermediates.     

Stabilization of native protein fold by intein-mediated covalent cyclization

A mutant version of the N-terminal domain of Escherichia coli DnaB helicase was used as a model system to assess the stabilization against unfolding gained by covalent cyclization. Cyclization was achieved in vivo by formation of an amide bond between the N and C termini with the help of a split mini-intein. Linear and circular proteins were constructed to be identical in amino acid sequence. Mutagenesis of Phe102 to Glu rendered the protein monomeric even at high concentration. A difference in free energy of unfolding, DeltaDeltaG, between circular and linear protein of 2.3(+/-0.5) kcal mol(-1) was measured at 10 degrees C by circular dichroism. A theoretical estimate of the difference in conformational entropy of linear and circular random chains in a three-dimensional cubic lattice model predicted DeltaDeltaG=2.3 kcal mol(-1), suggesting that stabilization by protein cyclization is driven by the reduced conformational entropy of the unfolded state. Amide-proton exchange rates measured by NMR spectroscopy and mass spectrometry showed a uniform, approximately tenfold decrease of the exchange rates of the most slowly exchanging amide protons, demonstrating that cyclization globally decreases the unfolding rate of the protein. The amide proton exchange was found to follow EX1 kinetics at near-neutral pH, in agreement with an unusually slow refolding rate of less than 4 min(-1) measured by stopped-flow circular dichroism. The linear and circular proteins differed more in their unfolding than in their folding rates. Global unfolding of the N-terminal domain of E.coli DnaB is thus promoted strongly by spatial separation of the N and C termini, whereas their proximity is much less important for folding.     

Kinetics of unfolding and folding from amide hydrogen exchange in native ubiquitin

Amide hydrogen (NH) exchange is one of the few experimental techniques with the potential for determining the thermodynamics and kinetics of conformational motions at nearly every residue in native proteins. Quantitative interpretation of NH exchange in terms of molecular motions relies on a simple two-state kinetic model: at any given slowly exchanging NH, a closed or exchange-incompetent conformation is in equilibrium with an open or exchange-competent conformation. Previous studies have demonstrated the accuracy of this model in measuring conformational equilibria by comparing exchange data with the thermodynamics of protein unfolding. We report here a test of the accuracy of the model in determining the kinetics of conformational changes in native proteins. The kinetics of folding and unfolding for ubiquitin have been measured by conventional methods and compared with those derived from a comprehensive analysis of the pH dependence of exchange in native ubiquitin. Rate constants for folding and unfolding from these two very different types of experiments show good agreement. The simple model for NH exchange thus appears to be a robust framework for obtaining quantitative information about molecular motions in native proteins.     

Unfolding and refolding of bovine beta-lactoglobulin monitored by hydrogen exchange measurements.

Bovine beta-lactoglobulin (beta-LG) is a widely studied protein belonging to the lipocalin family, whose structural characterisation has been reported by X-ray crystallography and NMR studies at physiological and acidic pH, respectively. Bovine beta-LG consists of nine antiparallel beta-sheets and a terminal alpha-helix segment. The beta-sheets form a calyx structure with a hydrophobic buried cluster conferring stability to the protein while a hydrophobic surface patch provides stabilising interactions between the barrel and the flanking terminal helix. Here, the stability and the folding properties of bovine beta-LG in the presence of a chemical denaturant is probed. The analysis of the NMR spectra recorded in aqueous solution with increasing amounts of urea revealed that the intensities of the backbone cross-peaks decrease upon increasing urea concentration, while their secondary shifts do not change significantly on going from 0 to 5 M urea, thus suggesting the presence of slow exchange between native and unfolded protein. Hydrogen exchange measurements at different urea concentrations were performed in order to evaluate the exchange rates of individual backbone amide protons. The opening reactions that determine protein exchange can be computed for the most slowly exchanging hydrogen atoms, and the measured exchange rates and the corresponding free energies can be expressed in terms of the equilibrium energetic for the global transition and the local fluctuations. Most of the residues converge to define a common isotherm identifying a unique cooperative folding unit, encompassing all the strands, except strand betaI, and the terminal region of the helix. The amides that do not join the same global unfolding isotherm are characterised by low DeltaGH20op and especially by low m values, indicating that they are already substantially exposed in the native state. A two-state unfolding model N <==> U is therefore proposed for this rather big protein, in agreement with CD data. Renaturation studies show that the unfolding mechanism is reversible up to 6 M urea and suggest a similar unfolding and refolding pathway. Present results are discussed in light of the hypothesis of an alpha-->beta transition proposed for bovine beta-LG refolding.     

Transient intermediates in the folding of dihydrofolate reductase as detected by far-ultraviolet circular dichroism spectroscopy

The kinetics of the reversible folding and unfolding of Escherichia coli dihydrofolate reductase have been studied by stopped-flow circular dichroism in the peptide region at pH 7.8 and 15 degrees C. The reactions were induced by concentration jumps of a denaturant, urea. The method can detect various intermediates transiently populated in the reactions although the equilibrium unfolding of the protein is apparently approximated by a two-state reaction. The results can be summarized as follows. (1) From transient circular dichroism spectra measured as soon as the refolding is started, a substantial amount of secondary structure is formed in the burst phase, i.e., within the dead time of stopped-flow mixing (18 ms). (2) The kinetics from this burst-phase intermediate to the native state are multiphasic, consisting of five phases designated as tau 1, tau 2, tau 3, tau 4, and tau 5 in increasing order of the reaction rate. Measurements of the kinetics at various wavelengths have provided kinetic difference circular dichroism spectra for the individual phases. (3) The tau 5 phase shows a kinetic difference spectrum consistent with an exciton contribution of two aromatic residues in the peptide CD region. The absence of the tau 5 phase in a mutant protein, in which Trp 74 is replaced by leucine, suggests that Trp 74 is involved in the exciton pair and that the tau 5 phase reflects the formation of a hydrophobic cluster around Trp 74. From the similarity of the kinetic difference spectrum to the difference between the native spectra of the mutant and wild-type proteins, it appears that Trp 47 is the partner in the exciton pair and that the structure formed in the tau 5 phase persists during the later stages of folding. (4) The later stages of folding show kinetic difference spectra that can be interpreted by rearrangement of secondary structure, particularly the central beta sheet of the protein. The pairwise similarities in the spectrum between the tau 3 and tau 4 phases, and between the tau 1 and tau 2 phases, also suggest the presence of two parallel folding channels for refolding. (5) The unfolding kinetics show three to four phases and are interpreted in terms of the presence of multiple native species. The total ellipticity change in kinetic unfolding reaction, however, agrees with the ellipticity difference between the native and unfolding states, indicating the absence of the burst phase in unfolding.(ABSTRACT TRUNCATED AT 400 WORDS)     

The equilibrium unfolding intermediate observed at pH 4 and its relationship with the kinetic folding intermediates in green fluorescent protein

Folding mechanisms of a variant of green fluorescent protein (F99S/M153T/V163A) were investigated by a wide variety of spectroscopic techniques. Equilibrium measurements on acid-induced denaturation of the protein monitored by chromophore and tryptophan fluorescence and small-angle X-ray scattering revealed that this protein accumulates at least two equilibrium intermediates, a native-like intermediate and an unfolding intermediate, the latter of which exhibits the characteristics of the molten globule state under moderately denaturing conditions at pH 4. To elucidate the role of the equilibrium unfolding intermediate in folding, a series of kinetic refolding experiments with various combinations of initial and final pH values, including pH 7.5 (the native condition), pH 4.0 (the moderately denaturing condition where the unfolding intermediate is accumulated), and pH 2.0 (the acid-denaturing condition) were carried out by monitoring chromophore and tryptophan fluorescence. Kinetic on-pathway intermediates were accumulated during the folding on the refolding reaction from pH 2.0 to 7.5. However, the signal change corresponding to the conversion from the acid-denatured to the kinetic intermediate states was significantly reduced on the refolding reaction from pH 4.0 to pH 7.5, whereas only the signal change corresponding to the above conversion was observed on the refolding reaction from pH 2.0 to pH 4.0. These results indicate that the equilibrium unfolding intermediate is composed of an ensemble of the folding intermediate species accumulated during the folding reaction, and thus support a hierarchical model of protein folding.     

Partially unfolded forms and non-two-state folding of a beta-sandwich: FHA domain from Arabidopsis receptor kinase-associated protein phosphatase

FHA domains adopt a beta-sandwich fold with 11 strands. The first evidence of partially unfolded forms of a beta-sandwich is derived from native-state hydrogen exchange (NHX) of the forkhead-associated (FHA) domain from kinase-associated protein phosphatase from Arabidopsis. The folding kinetics of this FHA domain indicate that EX2 behavior prevails at pH 6.3. In the chevron plot, rollover in the folding arm and bends in the unfolding arm suggest folding intermediates. NHX of this FHA domain suggests a core of six most stable beta-strands and two loops, characterized by rare global unfolding events. Flanking this stable core are beta-strands and recognition loops with less stability, termed subglobal motifs. These suggest partially unfolded forms (near-native intermediates) with two levels of stability. The spatial separation of the subglobal motifs on the flanks suggests possible parallelism in their folding as additional beta-strands align with the stable core of six strands. Intermediates may contribute to differences in stabilities and m-values suggested by NHX or kinetics relative to chemical denaturation. Residual structure in the unfolded regime is suggested by superprotection of beta-strand 6 and by GdmCl-dependence of adjustments in amide NMR spectra and residual optical signal. The global folding stability depends strongly on pH, with at least 3 kcal/mol more stability at pH 7.3 than at pH 6.3. This FHA domain is hypothesized to fold progressively with initial hydrophobic collapse of its stable six-stranded core followed by addition of less stable flanking beta-strands and ordering of recognition loops.