Oxidation of lysozyme by iodine: identification and properties of an oxindolyl ester intermediate: evidence for participation of glutamic acid 35 in catalysis

The first product formed in the iodine oxidation of tryptophan 108 of lysozyme has a transition temperature more than 20 deg. C higher than that of native and oxindolealanine 108-lysozyme. Irreversible rapid conversion to the oxindole follows unfolding. The spectrum of the oxidized residue of the intermediate resembles that of tryptophan. The iodine oxidation of tryptophan 108 is faster than that of N-acetyltryptophan ethyl ester. These and other aspects of the lysozyme-iodine reaction are explained by the formation, possibly concerted with oxidation, of the oxindolyl ester of glutamic acid 35. The data accord with results of high-resolution crystallographic analysis (Beddell &; Blake, 1970). Ester 108-lysozyme binds substrate like the native enzyme but retains less than 0.1% of the native activity. These results and the crystallographic data demonstrate catalytic function for glutamic acid 35. Oxindolealanine 108-lysozyme binds substrate only weakly. Introduction of an ester crosslink adds more than 6 kcal to the stability of lysozyme.     

Differences in the pathways for unfolding and hydrogen exchange among mutants of Escherichia coli alkaline phosphatase

Our initial studies of hydrogen-deuterium (H-D) exchange of tryptophan 109 in Escherichia coli alkaline phosphatase (AP) suggested that significant local unfolding of the protein might occur to allow for the exchange reaction, which is very slow at room temperature (Fischer et al., Biochemistry 39 (2000) 1455-1461). In order to investigate whether the partial unfolding and/or 'breathing' motions leading to H-D exchange were part of the unfolding pathway of the protein we prepared a series of mutants, designed to produce cavities around the exchanging residue, and compared their rates of H-D exchange to their lability (rate of inactivation) in guanidine hydrochloride (Gd:HCl). The complex unfolding kinetics of the mutants in the presence of Gd:HCl showed several components with rates that differed substantially among these proteins, but none of the rates of denaturation induced with Gd:HCl was consistently correlated with the H-D exchange rates. We conclude that the partial opening of the AP structure during the H-D exchange of tryptophan 109, although very slow, is not a rate determining step in the unfolding of this protein.     

Hydrogen exchange of the tryptophan residues in bovine alpha-lactalbumin studied by UV spectroscopy

The effect of Ca²⁺ ion on structural fluctuation of a milk Ca²⁺-binding protein, α-lactalbumin, under native conditions was investigated by comparing hydrogen-exchange reactions of tryptophan residues in the apo-form without Ca²⁺ and in the holo-form at 1 mM CaCl₂ at pH 7.0 in the presence of 0.1M Na⁺. The reactions were followed by measuring time-dependent absorption changes at 298–300 nm due to the ²H-¹H exchange of the tryptophan imino protons and were found to be biphasic under all the conditions examined. Two of the four tryptophan protons are insensitive to Ca²⁺ concentration and show a relatively fast exchange rate. The other two protons are much more extensively protected (a protection degree of 10³–10⁵) and are markedly affected by the presence of Ca²⁺. Examinations of the temperature dependence and pH dependence of the individual exchange rates have been utilized for elucidating the exchange mechanism. The fast protons show a low activation energy reaction with so-called EX₂ kinetics. The exchange reaction of the slow protons is accompanied by a high activation energy, and the exchange mechanism of the protons depended on the presence or absence of stabilizing Ca²⁺ ions—the EX₁ kinetics for the apo-protein and the EX₂ kinetics for the holo-protein at 1 mM Ca²⁺. The exchange reaction in the thermally unfolded state was also found to be biphasic, but the fast phase, which has an exchange rate in the fully exposed state, becomes predominant with decreasing temperature. By taking this fact and using a structural unfolding model of hydrogen exchange, the present results are fully consistent with thermodynamic parameters of the thermal transition and kinetic parameters of refolding reactions induced by concentration jumps of guanidine hydrochloride obtained in previous studies. It is demonstrated that the reaction of the slow protons in the native state is mediated by a transient global unfolding equivalent to the “thermal” unfolding under a native condition and that switching of the exchange mechanism from the EX₁ to EX₂ kinetics results from acceleration of the refolding rate with an increase in Ca²⁺ concentration. The transient global unfolding takes place even under a strongly native condition, e.g., at a temperature 20° below the beginning of the thermal transition.     

Comparison between the unfolding rate and structural fluctuations in native lysozyme--effects of denaturants, ligand binding, and intrachain cross-linking on hydrogen exchange and unfolding kinetics

The hydrogen-exchange reactions of peptide NH groups in lysozyme were studied by the change in the intensity of the amide II band in the ir spectrum. The slowest exchanging hydrogens, which are involved in intramolecular hydrogen bonding, are further divided into two groups at lower temperatures; half of them are exchanged through local unfolding and the other half through major cooperative unfolding. In order to study the correlation of the change in hydrogen-exchange rates with the change in the unfolding rate constant, we observed the effects of intrachain cross-linking, the addition of denaturant and ligand binding on the exchange rates through local unfolding. Although the exchange rate through major unfolding is greatly decreased by intrachain cross-linking between Glu 35 and Trp 108 (1/22000), the exchange rate through local unfolding is only slightly decreased (1/20). Even at higher temperatures, where most intact lysozyme molecules unfold, the folded conformation of cross-linked lysozyme remains compact, and no intermediate exists in which many side-chain atoms are packed loosely so that the hydrogen-exchange reaction occurs rapidly. Neither the addition of 2-PrOD molecules nor (NAG)₃ binding affects the exchange rates through local unfolding. Our experiments confirm that the change in the unfolding rate constant does not correlate with the change in fluctuations in the relatively flexible hydrogen-bonded structure through which the exchange of peptide hydrogens takes place.     

Gamma-irradiated chymotrypsin-like proteins. I. Structural changes.

The chymotrypsin-like proteins (chymotrypsin-CT,chymotrypsinogen-CTG, trypsin-T and modified chymotrypsins-at Met 192-MCT and at Tyr 146, 171-TCT), gamma-irradiated in the presence of air, were investigated. Irradiation leads to the unfolding of the native structure of CT-like proteins both in solution and in the dry state, which was shown by the tryptophan fluorescence, viscosimetry and microcalorimetry. The radiation yield of unfolded molecules Gconf was estimated and compared with (1) the rate constants for the reactions of OH-radicals with the proteins as determined by the p-nitrosodimethylaniline, (2) general stability of protein globule using the difference of the energies of the unfolded and globular conformations and (3) the radiation yield of tryptophan destruction in proteins-G-trp. There was a correlation between the values of Gconf and G-trp. The ratio G-trp/Gconf, which defines the number of destroyed tryptophan residues for one unfolded protein molecule, was constant within the limits of error. For CT, MCT, TCT and CTG, this ratio was on the average 3-2, and for T it was 2-2 residues. These facts point to the role of tryptophan destruction in the unfolding of the native structure of CT-like proteins on irradiation.     

Temperature-dependent downhill unfolding of ubiquitin. II. Modeling the free energy surface

To provide evidence for the interpretation of temperature‐dependent unfolding kinetics and the downhill unfolding scenario presented in the accompanying experimental article (Part I), the free energy surface of ubiquitin unfolding is calculated using statistical mechanical models of the Muñoz‐Eaton (ME) form. The models allow only two states for each amino acid residue, folded or unfolded, and permutations of these states generate an ensemble of microstates. One‐dimensional free energy curves are calculated using the number of folded residues as a reaction coordinate. The proposed sequential unfolding of ubiquitin's β‐sheet is tested by mapping the free energy onto two reaction coordinates inspired by the experiment as follows: the number of folded residues in ubiquitin's stable β‐strands I and II and those of the less stable strands III–V. Although the original ME model successfully captures folding features of zipper‐like one‐dimensional folders, it misses important tertiary interactions between residues that are far from each other in primary sequence. To take tertiary contacts into account, partially folded microstates based on a spherical growth model are included in the calculation and compared with the original model. By calculating the folding probability of each residue for a given point on the free energy surface, the unfolding pathway of ubiquitin is visualized. At low temperature, thermal unfolding occurs along a sequential unfolding pathway as follows: disruption of the β‐strands III–V followed by unfolding of the strands I and II. At high temperature, multiple unfolding routes are formed. The heterogeneity of the transition state explains the global nonexponential unfolding observed in the T‐jump experiment at high temperature. The calculation also reports a high stability for the α‐helix of ubiquitin. Proteins 2008. © 2008 Wiley‐Liss, Inc.     

Urea Impedes the Hydrophobic Collapse of Partially Unfolded Proteins

Proteins are denatured in aqueous urea solution. The nature of the molecular driving forces has received substantial attention in the past, whereas the question how urea acts at different phases of unfolding is not yet well understood at the atomic level. In particular, it is unclear whether urea actively attacks folded proteins or instead stabilizes unfolded conformations. Here we investigated the effect of urea at different phases of unfolding by molecular dynamics simulations, and the behavior of partially unfolded states in both aqueous urea solution and in pure water was compared. Whereas the partially unfolded protein in water exhibited hydrophobic collapses as primary refolding events, it remained stable or even underwent further unfolding steps in aqueous urea solution. Further, initial unfolding steps of the folded protein were found not to be triggered by urea, but instead, stabilized. The underlying mechanism of this stabilization is a favorable interaction of urea with transiently exposed, less-polar residues and the protein backbone, thereby impeding back-reactions. Taken together, these results suggest that, quite generally, urea-induced protein unfolding proceeds primarily not by active attack. Rather, thermal fluctuations toward the unfolded state are stabilized and the hydrophobic collapse of partially unfolded proteins toward the native state is impeded. As a result, the equilibrium is shifted toward the unfolded state.     

Escherichia coli OmpA retains a folded structure in the presence of sodium dodecyl sulfate due to a high kinetic barrier to unfolding.

Escherichia coli OmpA can be solubilized by sodium dodecyl sulfate (SDS) in its folded structure, and it unfolds upon heating. Although the heat-denatured OmpA remains unfolded after lowering the temperature, the addition of a non-ionic surfactant, octyl glucoside results in refolding of unfolded OmpA. In the present study, we investigated the refolding kinetics of OmpA in a mixed surfactant system of SDS and octyl glucoside using far- and near-UV circular dichroism and fluorescence spectroscopies. We found four kinetic phases in the refolding reaction, which logarithmically depended on the weight fraction of octyl glucoside. We also examined the unfolding kinetics of OmpA upon heating in the presence of SDS by temperature jump experiments. A comparison of the rate constants for the refolding and the unfolding reactions in SDS-only solution at 30 degrees C revealed that the folded form of OmpA in SDS solution is less stable than the unfolding form, and that the unfolding is virtually unobservable near room temperature due to a high kinetic barrier.     

Hydrogen exchange of the tryptophan residues in bovine, goat, guinea pig, and human alpha-lactalbumin

Hydrogen exchange of the individual tryptophan residues of bovine, goat, guinea pig, and human alpha-lactalbumin has been studied by both ultraviolet and NMR spectra. The assignment of the slowly exchanging imino proton resonances to the tryptophan residues (Trp26 and Trp60) was obtained by comparison of the nuclear Overhauser effect difference spectra of bovine, guinea pig, and human alpha-lactalbumin. Taking account of the thermal unfolding of each alpha-lactalbumin, the hydrogen exchange rates of the individual tryptophan residues are analyzed. The temperature dependence of the exchange rates classified their exchange mechanisms into two exchange processes: the "low activation energy process" and the "high activation energy process" which is associated directly with the global thermal unfolding of the protein. Trp26 of alpha-lactalbumin exchanges through the high activation energy process. The exchange behavior of Trp26 of guinea pig alpha-lactalbumin suggests a difference of the globally unfolded state of the protein from the other species. The exchange mechanism of Trp60 of human alpha-lactalbumin is the low activation energy process in contrast with those of the bovine and goat proteins, although their global thermodynamic properties are similar to each other. Trp104 and Trp118 of alpha-lactalbumin exchange through the low activation energy process, and the reaction rates are affected by the local structural differences around the tryptophan residues among these proteins. The results presented in this paper indicate that the hydrogen exchange rate through the low activation energy process provides the information only about the local nature of a protein while that through the high activation energy process provides the information about the global nature of a protein.     

Microsecond simulations of the folding/unfolding thermodynamics of the Trp‐cage miniprotein

We study the unbiased folding/unfolding thermodynamics of the Trp‐cage miniprotein using detailed molecular dynamics simulations of an all‐atom model of the protein in explicit solvent using the Amberff99SB force field. Replica‐exchange molecular dynamics simulations are used to sample the protein ensembles over a broad range of temperatures covering the folded and unfolded states at two densities. The obtained ensembles are shown to reach equilibrium in the 1 μs/replica timescale. The total simulation time used in the calculations exceeds 100 μs. Ensemble averages of the fraction folded, pressure, and energy differences between the folded and unfolded states as a function of temperature are used to model the free energy of the folding transition, ΔG(P, T), over the whole region of temperatures and pressures sampled in the simulations. The ΔG(P, T) diagram describes an ellipse over the range of temperatures and pressures sampled, predicting that the system can undergo pressure‐induced unfolding and cold denaturation at low temperatures and high pressures, and unfolding at low pressures and high temperatures. The calculated free energy function exhibits remarkably good agreement with the experimental folding transition temperature (T_f = 321 K), free energy, and specific heat changes. However, changes in enthalpy and entropy are significantly different than the experimental values. We speculate that these differences may be due to the simplicity of the semiempirical force field used in the simulations and that more elaborate force fields may be required to describe appropriately the thermodynamics of proteins. Proteins 2010. © 2010 Wiley‐Liss, Inc.     

Conformational dynamics of the GdmHCl-induced molten globule state of creatine kinase monitored by hydrogen exchange and mass spectrometry

Our understanding of the mechanism of protein folding can be improved by the characterization of folding intermediate states. Intrinsic tryptophan fluorescence measurements of equilibrium GdmHCl-induced unfolding of MM-CK allow for the construction of a "phase diagram", which shows the presence of five different conformational states, including three partially folded intermediates. However, only three states are detected by using pulsed-labeled H-D exchange analyzed by electrospray ionization mass spectrometry. One of them is the native state, and the two other species are present in proportions strongly dependent on the GdmHCl concentration and denaturation time. The low-mass peak is due to a largely exchange-incompetent state, which has gained only approximately 10 deuteriums more than the native protein. This population of MM-CK molecules has undergone a small conformational change induced by low GdmHCl concentrations. However, this limited change is in itself not sufficient to inactivate the enzyme or is easily reversible. The high-mass peak corresponds to a population of MM-CK that is fully deuterated. The comparison of fluorescence, activity, and H-D exchange measurements shows that the maximally populated intermediate at 0.8 M GdmHCl has the characteristics of a molten globule. It has no activity; it has 55% of its native alpha-helices and a maximum fluorescence emission wavelength of approximately 341 nm, and it binds ANS strongly. However, no protection against exchange is detected under the conditions used in this work. This paradox, the presence of significant residual secondary and tertiary structures detected by optical probes and the total deuteration of its amide protons detected by H-D exchange and mass spectrometry, could be explained by a highly dynamic MM-CK molten globule.     

Pressure-jump studies of the folding/unfolding of trp repressor.

The dimeric protein, trp apo-repressor of Escherichia coli has been subjected to high hydrostatic pressure under a variety of conditions, and the effects have been monitored by fluorescence spectroscopic and infra-red absorption techniques. Under conditions of micromolar protein concentration and low, non-denaturing concentrations of guanidinium hydrochloride (GuHCl), tryptophan and 8-anilino-1-naphthalene sulfonate (ANS) fluorescence detected high pressure profiles demonstrate that pressures below 3 kbar result in dissociation of the dimer to a monomeric species that presents no hydrophobic binding sites for ANS. The FTIR-detected high pressure profile obtained under significantly different solution conditions (30 mM trp repressor in absence of denaturant) exhibits a much smaller pressure dependence than the fluorescence detected profiles. The pressure-denatured form obtained under the FTIR conditions retains about 50 % alpha-helical structure. From this we conclude that the secondary structure present in the high pressure state achieved under the conditions of the fluorescence experiments is at least as disrupted as that achieved under FTIR conditions. Fluorescence-detected pressure-jump relaxation studies in the presence of non-denaturing concentrations of GuHCl reveal a positive activation volume for the association/folding reaction and a negative activation volume for dissociation/unfolding reaction, implicating dehydration as the rate-limiting step for association/folding and hydration as the rate-limiting step for unfolding. The GuHCl concentration dependence of the kinetic parameters place the transition state at least half-way along the reaction coordinate between the unfolded and folded states. The temperature dependence of the pressure-jump fluorescence-detected dissociation/unfolding reaction in the presence of non-denaturing GuHCl suggests that the curvature in the temperature dependence of the stability arises from non-Arrhenius behavior of the folding rate constant, consistent with a large decrease in heat capacity upon formation of the transition state from the unfolded state. The decrease in the equilibrium volume change for folding with increasing temperature (due to differences in thermal expansivity of the folded and unfolded states) arises from a decrease in the absolute value for the activation volume for unfolding, thus indicating that the thermal expansivity of the transition state is similar to that of the unfolded state.     

Detection of intermediates in protein folding of carbonic anhydrase with fluorescence emission and polarization.

The three-dimensional structure of carbonic anhydrase is a result of specific folding of the protein chain to form a compact, globular molecule. Fluorescence measurements on the nature of the rate-limiting steps in folding from the random coil to the native structure show that each step involves an actual folding reaction of the protein chain. Emission intensity and polarization of the intrinsic fluorescence due to tryptophan residues reach a maximum during the early period of the folding process. The changes occur in at least three kinetic phases (tau1 less than 3 S, tau2 = 1 min, tau3 = 10 min, 1 M guanidinium chloride, 2 M NaC1, pH 7, 20 degrees C). None of these phases are explained by configurational changes in the fully unfolded chain. The results are consistent with a kinetic scheme that involves stepwise acquisition of the specific folded structure of the native enzyme.     

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.     

Probing the role of the F-helix in serpin stability through a single tryptophan substitution

Serpins form loop-sheet polymers through the formation of a partially folded intermediate. Through mutagenesis and biophysical analysis, we have probed the conformational stability of the F-helix, demonstrating that it is almost completely unfolded in the intermediate state. The replacement of Tyr160 on the F-helix of alpha1-antitrypsin to alanine results in the loss of a conserved hydrogen bond that dramatically reduces the stability of the protein to both heat and solvent denaturation, indicating the importance of Tyr160 in the stability of the molecule. The mutation of Tyr160 to a tryptophan residue, within a fluorescently silent variant of alpha1-antitrypsin, results in a fully active, stable serpin. Fluorescence analysis of the equilibrium unfolding behavior of this variant indicates that the F-helix is highly disrupted in the intermediate conformation. Iodide quenching experiments demonstrate that the tryptophan residue is exposed to a similar extent in both the intermediate and unfolded states. Cumulatively, these data indicate that the F-helix plays an important role in controlling the early conformational changes involved in alpha1-antitrypsin unfolding. The implications of these data on both alpha1-antitrypsin function and misfolding are discussed.     

Determination of ultrafast protein folding rates from loop formation dynamics

Quenching of the triplet state of tryptophan by contact with cysteine can be used to measure the kinetics of loop formation in unfolded proteins. Here we show that cysteine quenching dynamics also provide a novel method for measuring folding rates when the exchange between folded and unfolded states is faster than the unquenched triplet lifetime (approximately 100 micros). We use this technique to investigate folding/unfolding kinetics of the 35 residue headpiece subdomain of the protein villin, which contains a single tryptophan residue and was engineered to contain a cysteine residue at the N terminus. At intermediate concentrations of denaturant the time-course of the triplet decay consists of two relaxations, the rates and amplitudes of which reveal the fast kinetics for folding and unfolding of this protein. The folding rates extracted using a simple kinetic model are close to those reported previously from laser-induced temperature-jump experiments that employ the change in tryptophan fluorescence as a probe. However, the results differ significantly from those reported from dynamic NMR line shape analysis on a variant with methionine at the N terminus, an issue that remains to be resolved. The analysis of the triplet quenching kinetics also shows that the quenching rates in the unfolded state increase with decreasing denaturant concentration, indicating a compaction of the unfolded protein.     

Characterization of the folding and unfolding reactions of single-chain monellin: evidence for multiple intermediates and competing pathways

The mechanisms of folding and unfolding of the small plant protein monellin have been delineated in detail. For this study, a single-chain variant of the natively two-chain monellin, MNEI, was used, in which the C terminus of chain B was connected to the N terminus of chain A by a Gly-Phe linker. Equilibrium guanidine hydrochloride (GdnHCl)-induced unfolding experiments failed to detect any partially folded intermediate that is stable enough to be populated at equilibrium to a significant extent. Kinetic experiments in which the refolding of GdnHCl-unfolded protein was monitored by measurement of the change in the intrinsic tryptophan fluorescence of the protein indicated the accumulation of three transient partially structured folding intermediates. The fluorescence change occurred in three kinetic phases: very fast, fast, and slow. It appears that the fast and slow changes in fluorescence occur on competing folding pathways originating from one unfolded form and that the very fast change in fluorescence occurs on a third parallel pathway originating from a second unfolded form of the protein. Kinetic experiments in which the refolding of alkali-unfolded protein was monitored by the change in the fluorescence of the hydrophobic dye 8-anilino-1-naphthalenesulfonic acid (ANS), consequent to the dye binding to the refolding protein, as well as by the change in intrinsic tryptophan fluorescence, not only confirmed the presence of the three kinetic intermediates but also indicated the accumulation of one or more early intermediates at a few milliseconds of refolding. These experiments also exposed a very slow kinetic phase of refolding, which was silent to any change in the intrinsic tryptophan fluorescence of the protein. Hence, the spectroscopic studies indicated that refolding of single-chain monellin occurs in five distinct kinetic phases. Double-jump, interrupted-folding experiments, in which the accumulation of folding intermediates and native protein during the folding process could be determined quantitatively by an unfolding assay, indicated that the fast phase of fluorescence change corresponds to the accumulation of two intermediates of differing stabilities on competing folding pathways. They also indicated that the very slow kinetic phase of refolding, identified by ANS binding, corresponds to the formation of native protein. Kinetic experiments in which the unfolding of native protein in GdnHCl was monitored by the change in intrinsic tryptophan fluorescence indicated that this change occurs in two kinetic phases. Double-jump, interrupted-unfolding experiments, in which the accumulation of unfolding intermediates and native protein during the unfolding process could be determined quantitatively by a refolding assay, indicated that the fast unfolding phase corresponds to the formation of fully unfolded protein via one unfolding pathway and that the slow unfolding phase corresponds to a separate unfolding pathway populated by partially unfolded intermediates. It is shown that the unfolded form produced by the fast unfolding pathway is the one which gives rise to the very fast folding pathway and that the unfolded form produced by the slower unfolding pathway is the one which gives rise to the slow and fast folding pathways.     

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.     

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.