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.     

Equilibrium unfolding of dimeric and engineered monomeric forms of lambda Cro (F58W) repressor and the effect of added salts: evidence for the formation of folded monomer induced by sodium perchlorate

The equilibrium unfolding transitions of Cro repressor variants, dimeric variant Cro F58W and monomer Cro K56[DGEVK]F58W, have been studied by urea and guanidine hydrochloride to probe the folding mechanism. The unfolding transitions of a dimeric variant are well described by a two state process involving native dimer and unfolded monomer with a free energy of unfolding, DeltaG(0,un)(0), of approximately 10-11 kcal/mol. The midpoint of transition curves is dependent on total protein concentration and DeltaG(0,un)(0) is independent of protein concentration, as expected for this model. Unfolding of Cro monomer is well described by the standard two state model. The stability of both forms of protein increases in the presence of salt but decreases with the decrease in pH. Because of the suggested importance of a N2<-->2F dimerization process in DNA binding, we have also studied the effect of sodium perchlorate, containing the chaotropic perchlorate anion, on the conformational transition of Cro dimer by CD, fluorescence and NMR (in addition to urea and guanidine hydrochloride) in an attempt both to characterize the thermodynamics of the process and to identify conditions that lead to an increase in the population of the folded monomers. Data suggest that sodium perchlorate stabilizes the protein at low concentration (<1.5 M) and destabilizes the protein at higher perchlorate concentration with the formation of a "significantly folded" monomer. The tryptophan residue in the "significantly folded" monomer induced by perchlorate is more exposed to the solvent than in native dimer.     

Linked thermal and solute perturbation analysis of cooperative domain interactions in proteins. Structural stability of diphtheria toxin

The temperature and guanidine hydrochloride (GuHCl) dependence of the structural stability of diphtheria toxin has been investigated by high-sensitivity differential scanning calorimetry. In 50 mM phosphate buffer at pH 8.0 and in the absence of GuHCl, the thermal unfolding of diphtheria toxin is characterized by a transition temperature (Tm) of 54.9 degrees C, a calorimetric enthalpy change (delta H) of 295 kcal/mol, and a van't Hoff to calorimetric enthalpy ratio of 0.57. Increasing the GuHCl concentration lowers the transition temperature and the calorimetric enthalpy change. At the same time, the van't Hoff to calorimetric enthalpy ratio increases until it reaches a value of 1 at 0.3 M GuHCl and remains constant thereafter. At low GuHCl concentrations (0-0.3 M), the thermal unfolding of diphtheria toxin is characterized by the presence of two transitions corresponding to the A and B domains of the protein. At higher GuHCl concentrations (0.3-1 M), the A domain is unfolded at all temperatures, and only one transition corresponding to the B domain is observed. Under these conditions, the most stable protein conformation at low temperatures is a partially folded state in which the A domain is unfolded and the B domain folded. A general model that explicitly considers the energetics of domain interactions has been developed in order to account for the stability and cooperative behavior of diphtheria toxin. It is shown that this cooperative domain interaction model correctly accounts for the temperature location as well as the shape and area of the calorimetric curves. Under physiological conditions, domain-domain interactions account for most of the structural stability of the A domain.(ABSTRACT TRUNCATED AT 250 WORDS)     

Folding is coupled to dimerization of Tctex-1 dynein light chain

Equilibrium analyses have been performed to elucidate the role of dimerization in folding and stability of dynein light chain Tctex-1. The equilibrium unfolding transition was monitored by intrinsic fluorescence intensity, fluorescence anisotropy, and circular dichroism and was modeled as a two-state mechanism where a folded dimer dissociates to two unfolded monomers without populating thermodynamically stable monomeric or dimeric intermediates. Sedimentation equilibrium and chemical cross-linking experiments performed at increasing concentrations of denaturants show no change in the association state before the unfolding transition and are consistent with the two-state model of dissociation coupled to unfolding. A linear dependence on denaturant concentration is observed by fluorescence intensity and anisotropy before unfolding in the 0-2 M GdnCl, and 0-4 M urea concentration range. This change is not protein concentration-dependent and possibly reflects relief of quenching associated with premelting conformational disorder in the vicinity of Trp 83. The data clearly show that the dissociation-coupled unfolding mechanism of Tctex-1 is different from the three-state denaturation mechanism of its structural homologue light chain LC8. The absence of a stable monomer in Tctex-1 offers insight into its functional differences from LC8.     

Mapping the folding free energy surface for metal-free human Cu,Zn superoxide dismutase

Mutations at many different sites in the gene encoding human Cu,Zn superoxide dismutase (SOD) are known to be causative agents in amyotrophic lateral sclerosis (ALS). One explanation for the molecular basis of this pathology is the aggregation of marginally soluble, partially structured states whose populations are enhanced in the protein variants. As a benchmark for testing this hypothesis, the equilibrium and kinetic properties of the reversible folding reaction of a metal-free variant of SOD were investigated. Reversibility was achieved by replacing the two non-essential cysteine residues with non-oxidizable analogs, C6A/C111S, to produce apo-AS-SOD. The metal-free pseudo-wild-type protein is folded and dimeric in the absence of chemical denaturants, and its equilibrium folding behavior is well described by an apparent two-state mechanism involving the unfolded monomer and the native dimer. The apparent free energy of folding in the absence of denaturant and at standard state is -20.37(+/- 1.04) kcal (mol dimer)(-1). A global analysis of circular dichroism kinetic traces for both unfolding and refolding reactions, combined with results from small angle X-ray scattering and time-resolved fluorescence anisotropy measurements, supports a sequential mechanism involving the unfolded monomer, a folded monomeric intermediate, and the native dimer. The rate-limiting monomer folding reaction is followed by a near diffusion-limited self-association reaction to form the native dimer. The relative population of the folded monomeric intermediate is predicted not to exceed 0.5% at micromolar concentrations of protein under equilibrium and both strongly unfolding and refolding conditions for metal-free pseudo-wild-type SOD.     

Equilibrium unfolding of a small low-potential cytochrome, cytochrome c553 from Desulfovibrio vulgaris.

To understand general aspects of stability and folding of c-type cytochromes, we have studied the folding characteristics of cytochrome c553 from Desulfovibrio vulgaris (Hildenborough). This cytochrome is structurally similar but lacks sequence homology to other heme proteins; moreover, it has an abnormally low reduction potential. Unfolding of oxidized and reduced cytochrome c553 by guanidine hydrochloride (GuHCl) was monitored by circular dichroism (CD) and Soret absorption; the same unfolding curves were obtained with both methods supporting that cytochrome c553 unfolds by an apparent two-state process. Reduced cytochrome c553 is 7(3) kJ/mol more stable than the oxidized form; accordingly, the reduction potential of unfolded cytochrome c553 is 100(20) mV more negative than that of the folded protein. In contrast to many other unfolded cytochrome c proteins, upon unfolding at pH 7.0 both oxidized and reduced heme in cytochrome c553 become high-spin. The lack of heme misligation in unfolded cytochrome c553 implies that its unfolded structure is less constrained than those of cytochromes c with low-spin, misligated hemes.     

Refolding of the hyperthermophilic protein Ssh10b involves a kinetic dimeric intermediate

The α/β-mixed dimeric protein Ssh10b from the hyperthermophile Sulfolobus shibatae is a member of the Sac10b family that is thought to be involved in chromosomal organization or DNA repair/recombination. The equilibrium unfolding/refolding of Ssh10b induced by denaturants and heat was fully reversible, suggesting that Ssh10b could serve as a good model for folding/unfolding studies of protein dimers. Here, we investigate the folding/unfolding kinetics of Ssh10b in detail by stopped-flow circular dichroism (SF-CD) and using GdnHCl as denaturant. In unfolding reactions, the native Ssh10b turned rapidly into fully unfolded monomers within the stopped-flow dead time with no detectable kinetic intermediate, agreeing well with the results of equilibrium unfolding experiments. In refolding reactions, two unfolded monomers associate in the burst phase to form a dimeric intermediate that undergoes a further, slower, first-order folding process to form the native dimer. Our results demonstrate that the dimerization is essential for maintaining the native tertiary interactions of the protein Ssh10b. In addition, folding mechanisms of Ssh10b and several other α/β-mixed or pure β-sheet proteins are compared.     

Mechanistic studies of the folding of human lysozyme and the origin of amyloidogenic behavior in its disease-related variants.

The unfolding and refolding properties of human lysozyme and two amyloidogenic variants (Ile56Thr and Asp67His) have been studied by stopped-flow fluorescence and hydrogen exchange pulse labeling coupled with mass spectrometry. The unfolding of each protein in 5.4 M guanidine hydrochloride (GuHCl) is well described as a two-state process, but the rates of unfolding of the Ile56Thr variant and the Asp67His variant in 5.4 M GuHCl are ca. 30 and 160 times greater, respectively, than that of the wild type. The refolding of all three proteins in 0.54 M GuHCl at pH 5.0 proceeds through persistent intermediates, revealed by multistep kinetics in fluorescence experiments and by the detection of well-defined populations in quenched-flow hydrogen exchange experiments. These findings are consistent with a predominant mechanism for refolding of human lysozyme in which one of the structural domains (the alpha-domain) is formed in two distinct steps and is followed by the folding of the other domain (the beta-domain) prior to the assembly of the two domains to form the native structure. The refolding kinetics of the Asp67His variant are closely similar to those of the wild-type protein, consistent with the location of this mutation in an outer loop of the beta-domain which gains native structure only toward the end of the refolding process. By contrast, the Ile56Thr mutation is located at the base of the beta-domain and is involved in the domain interface. The refolding of the alpha-domain is unaffected by this substitution, but the latter has the effect of dramatically slowing the folding of the beta-domain and the final assembly of the native structure. These studies suggest that the amyloidogenic nature of the lysozyme variants arises from a decrease in the stability of the native fold relative to partially folded intermediates. The origin of this instability is different in the two variants, being caused in one case primarily by a reduction in the folding rate and in the other by an increase in the unfolding rate. In both cases this results in a low population of soluble partially folded species that can aggregate in a slow and controlled manner to form amyloid fibrils.     

Thermodynamic characterization of nucleoplasmin unfolding: interplay between function and stability

The unfolding equilibrium of recombinant (rNP) and natural variants of nucleoplasmin (NP) from Xenopus laevis has been analyzed using biochemical and spectroscopic techniques. In the presence of denaturing concentrations of guanidinium salts (GuHCl and GuSCN), both domains, core and tail, of the rNP pentamer unfold as proven using single-carrying tryptophan mutants, whereas urea is remarkably unable to fully unfold rNP. Chemical unfolding is reversible and can be described well as a two-state transition in which the folded pentamer is directly converted to unfolded monomers, with no evidence of (partially) folded monomers. Therefore, rNP dissociates and fully unfolds simultaneously (N 5 <--> 5U). Activation of the protein by hyperphosphorylation is accompanied by a destabilization of the protein oligomer. A comparison of natural NP forms isolated from eggs and oocytes of X. laevis and recombinant NP reveals that natural variants can be fully unfolded by urea and exhibit D 50 (denaturant concentration at the transition midpoint) values lower than that of the nonphosphorylated protein. Progressive phosphorylation of NP correlates with a gradual loss of stability of 6 kcal/mol (oNP) and 10 kcal/mol (eNP), as compared with the nonphosphorylated protein pentamer. These results suggest that the remarkable stability of the recombinant protein is required to cope with the destabilization brought about by its phosphorylation-induced activation.     

Folding and unfolding of gammaTIM monomers and dimers

Kinetic simulations of the folding and unfolding of triosephosphate isomerase (TIM) from yeast were conducted using a single monomer gammaTIM polypeptide chain that folds as a monomer and two gammaTIM chains that fold to the native dimer structure. The basic protein model used was a minimalist Gō model using the native structure to determine attractive energies in the protein chain. For each simulation type--monomer unfolding, monomer refolding, dimer unfolding, and dimer refolding--thirty simulations were conducted, successfully capturing each reaction in full. Analysis of the simulations demonstrates four main conclusions. First, all four simulation types have a similar "folding order", i.e., they have similar structures in intermediate stages of folding between the unfolded and folded state. Second, despite this similarity, different intermediate stages are more or less populated in the four different simulations, with 1), no intermediates populated in monomer unfolding; 2), two intermediates populated with beta(2)-beta(4) and beta(1)-beta(5) regions folded in monomer refolding; 3), two intermediates populated with beta(2)-beta(3) and beta(2)-beta(4) regions folded in dimer unfolding; and 4), two intermediates populated with beta(1)-beta(5) and beta(1)-beta(5) + beta(6) + beta(7) + beta(8) regions folded in dimer refolding. Third, simulations demonstrate that dimer binding and unbinding can occur early in the folding process before complete monomer-chain folding. Fourth, excellent agreement is found between the simulations and MPAX (misincorporation proton alkyl exchange) experiments. In total, this agreement demonstrates that the computational Gō model is accurate for gammaTIM and that the energy landscape of gammaTIM appears funneled to the native state.     

Folding and stability of trp aporepressor from Escherichia coli

Equilibrium and kinetic studies of the urea-induced unfolding of trp aporepressor from Escherichia coli were performed to probe the folding mechanism of this intertwined, dimeric protein. The equilibrium unfolding transitions at pH 7.6 and 25 degrees C monitored by difference absorbance, fluorescence, and circular dichroism spectroscopy are coincident within experimental error. All three transitions are well described by a two-state model involving the native dimer and the unfolded monomer; the free energy of folding in the absence of denaturant and under standard-state conditions is estimated to be 23.3 +/- 0.9 kcal/mol of dimer. The midpoint of the equilibrium unfolding transition increases with increasing protein concentration in the manner expected from the law of mass action for the two-state model. We find no evidence for stable folding intermediates. Kinetic studies reveal that unfolding is governed by a single first-order reaction whose relaxation time decreases exponentially with increasing urea concentration and also decreases with increasing protein concentration in the transition zone. Refolding involves at least three phases that depend on both the protein concentration and the final urea concentration in a complex manner. The relaxation time of the slowest of these refolding phases is identical with that for the single phase in unfolding in the transition zone, consistent with the results expected for a reaction that is kinetically reversible. The two faster refolding phases are presumed to arise from slow isomerization reactions in the unfolded form and reflect parallel folding channels.     

Equilibrium dissociation and unfolding of the dimeric human papillomavirus strain-16 E2 DNA-binding domain.

The equilibrium unfolding reaction of the C-terminal 80-amino-acid dimeric DNA-binding domain of human papillomavirus (HPV) strain 16 E2 protein has been investigated using fluorescence, far-UV CD, and equilibrium sedimentation. The stability of the HPV-16 E2 DNA-binding domain is concentration-dependent, and the unfolding reaction is well described as a two-state transition from folded dimer to unfolded monomer. The conformational stability of the protein, delta GH2O, was found to be 9.8 kcal/mol at pH 5.6, with the corresponding equilibrium unfolding/dissociation constant, Ku, being 6.5 x 10(-8) M. Equilibrium sedimentation experiments give a Kd of 3.0 x 10(-8) M, showing an excellent agreement between the two different techniques. Denaturation by temperature followed by the change in ellipticity also shows a concomitant disappearance of secondary and tertiary structures. The Ku changes dramatically at physiologically relevant pH's: with a change in pH from 6.1 to 7.0, it goes from 5.5 x 10(-8) M to 4.4 x 10(10) M. Our results suggest that, at the very low concentration of protein where DNA binding is normally measured (e.g., 10(-11) M), the protein is predominantly monomeric and unfolded. They also stress the importance of the coupling between folding and DNA binding.     

In vitro unfolding,refolding, and polymerization of human gammaD crystallin,a protein involved in cataract formation

Human gammaD crystallin (HgammaD-Crys), a major protein of the human eye lens, is a primary component of cataracts. This 174-residue primarily beta-sheet protein is made up of four Greek keys separated into two domains. Mutations in the human gene sequence encoding HgammaD-Crys are implicated in early-onset cataracts in children, and the mutant protein expressed in Escherichia coli exhibits properties that reflect the in vivo pathology. We have characterized the unfolding, refolding, and competing aggregation of human wild-type HgammaD-Crys as a function of guanidinium hydrochloride (GuHCl) concentration at neutral pH and 37 degrees C, using intrinsic tryptophan fluorescence to monitor in vitro folding. Wild-type HgammaD-Crys exhibited reversible refolding above 1.0 M GuHCl. The GuHCl unfolded protein was more fluorescent than its native counterpart despite the absence of metal or ion-tryptophan interactions. Aggregation of refolding intermediates of HgammaD-Crys was observed in both equilibrium and kinetic refolding processes. The aggregation pathway competed with productive refolding at denaturant concentrations below 1.0 M GuHCl, beyond the major conformational transition region. Atomic force microscopy of samples under aggregating conditions revealed the sequential appearance of small nuclei, thin protofibrils, and fiber bundles. The HgammaD-Crys fibrous aggregate species bound bisANS appreciably, indicating the presence of exposed hydrophobic pockets. The mechanism of HgammaD-Crys aggregation may provide clues to understanding age-onset cataract formation in vivo.     

Molecular basis of cooperativity in protein folding IV. Core: A general cooperative folding model

The cooperative nature of the protein folding process is independent of the characteristic fold and the specific secondary structure attributes of a globular protein. A general folding/unfolding model should, therefore, be based upon structural features that transcend the peculiarities of α-helices, β-sheets, and other structural motifs found in proteins. The studies presented in this paper suggest that a single structural characteristic common to all globular proteins is essential for cooperative folding. The formation of a partly folded state from the native state results in the exposure to solvent of two distinct regions: (1) the portions of the protein that are unfolded; and (2) the “complementary surfaces,” located in the regions of the protein that remain folded. The cooperative character of the folding/unfolding transition is determined largely by the energetics of exposing complementary surface regions to the solvent. By definition, complementary regions are present only in partly folded states; they are absent from the native and unfolded states. An unfavorable free energy lowers the probability of partly folded states and increases the cooperativity of the transition. In this paper we present a mathematical formulation of this behavior and develop a general cooperative folding/unfolding model, termed the “complementary region” (CORE) model. This model successfully reproduces the main properties of folding/unfolding transitions without limiting the number of partly folded states accessible to the protein, thereby permitting a systematic examination of the structural and solvent conditions under which intermediates become populated. It is shown that the CORE model predicts two-state folding/unfolding behavior, even though the two-state character is not assumed in the model. © 1993 Wiley-Liss, Inc.     

Hydrogen exchange in a large 29 kD protein and characterization of molten globule aggregation by NMR

The nature of denatured ensembles of the enzyme human carbonic anhydrase (HCA) has been extensively studied by various methods in the past. The protein constitutes an interesting model for folding studies that does not unfold by a simple two-state transition, instead a molten globule intermediate is highly populated at 1.5 M GuHCl. In this work, NMR and H/D exchange studies have been conducted on one of the isozymes, HCA I. The H/D exchange studies, which were enabled by the previously obtained resonance assignment of HCA I, have been used to identify unfolded forms that are accessible from the native state. In addition, the GuHCl-induced unfolded states of HCA I have also been characterized by NMR at GuHCl concentrations in the 0-5 M range. The most important findings in this work are as follows: (1) Amide protons located in the center of the beta-sheet require global unfolding events for efficient H/D exchange. (2) The molten globule and the native state give similar protection against H/D exchange for all of the observable amide protons (i.e., water seems not to efficiently penetrate the interior of the molten globule). (3) At high protein concentrations, the molten globule can form large aggregates, which are not detectable by solution-state NMR methods. (4) The unfolded state (U), present at GuHCl concentrations above 2 M, is composed of an ensemble of conformations having residual structures with different stabilities.     

The V108M mutation decreases the structural stability of catechol O-methyltransferase

The human gene for catechol O-methyltransferase has a common single-nucleotide polymorphism that results in substitution of methionine (M) for valine (V) 108 in the soluble form of the enzyme (s-COMT). 108M s-COMT loses enzymatic activity more rapidly than 108V s-COMT at physiological temperature, and the 108M allele has been associated with increased risk of breast cancer and several neuropsychiatric disorders. We used circular dichroism (CD), dynamic light scattering, and fluorescence spectroscopy to examine how the 108V/M polymorphism affects the stability of the purified, recombinant protein to heat and guanidine hydrochloride (GuHCl). COMT contains two tryptophan residues, W143 and W38Y, which are located in loops that border the S-adenosylmethionine (SAM) and catechol binding sites. We therefore also studied the single-tryptophan mutants W38Y and W143Y in order to dissect the contributions of the individual tryptophans to the fluorescence signals. The 108V and 108M proteins differed in the stability of both the tertiary structure surrounding the active site, as probed by the fluorescence yields and emission spectra, and their global secondary structure as reflected by CD. With either probe, the midpoint of the thermal transition of 108M s-COMT was 5 to 7 degrees C lower than that of 108V s-COMT, and the free energy of unfolding at 25 degrees C was smaller by about 0.4 kcal/mol. 108M s-COMT also was more prone to aggregation or partial unfolding to a form with an increased radius of hydration at 37 degrees C. The co-substrate SAM stabilized the secondary structure of both 108V and 108M s-COMT. W143 dominates the tryptophan fluorescence of the folded protein and accounts for most of the decrease in fluorescence that accompanies unfolding by GuHCl. While replacing either tryptophan by tyrosine was mildly destabilizing, the lower stability of the 108M variant was retained in all cases.     

Using fluorescence correlation spectroscopy to study conformational changes in denatured proteins

Fluorescence correlation spectroscopy (FCS) is a sensitive analytical tool that allows dynamics and hydrodynamics of biomolecules to be studied under a broad range of experimental conditions. One application of FCS of current interest is the determination of the size of protein molecules in the various states they sample along their folding reaction coordinate, which can be accessed through the measurement of diffusion coefficients. It has been pointed out that the analysis of FCS curves is prone to artifacts that may lead to erroneous size determination. To set the stage for FCS studies of unfolded proteins, we first show that the diffusion coefficients of small molecules as well as proteins can be determined accurately even in the presence of high concentrations of co-solutes that change the solution refractive index significantly. Indeed, it is found that the Stokes-Einstein relation between the measured diffusion coefficient and solution viscosity holds even in highly concentrated glycerol or guanidinium hydrochloride (GuHCl) solutions. These measurements form the basis for an investigation of the structure of the denatured state of two proteins, the small protein L and the larger, three-domain protein adenylate kinase (AK). FCS is found useful for probing expansion in the denatured state beyond the unfolding transition. It is shown that the denatured state of protein L expands as the denaturant concentration increases, in a process akin to the transition from a globule to a coil in polymers. This process continues at least up to 5 M GuHCl. On the other hand, the denatured state of AK does not seem to expand much beyond 2 M GuHCl, a result that is in qualitative accord with single-molecule fluorescence histograms. Because both the unfolding transition and the coil-globule transition of AK occur at a much lower denaturant concentration than those of protein L, a possible correlation between the two phenomena is suggested.     

Equilibrium and kinetic analysis of folding of ketosteroid isomerase from Comamonas testosteroni

Equilibrium and kinetic analyses have been carried out to elucidate the folding mechanism of homodimeric ketosteroid isomerase (KSI) from Comamonas testosteroni. The folding of KSI was reversible since the activity as well as the fluorescence and CD spectra was almost completely recovered after refolding. The equilibrium unfolding transitions monitored by fluorescence and CD measurements were almost coincident with each other, and the transition midpoint increased with increasing protein concentration. This suggests that the KSI folding follows a simple two-state mechanism consisting of native dimer and unfolded monomer without any thermodynamically stable intermediates. Sedimentation equilibrium analysis and size-exclusion chromatography of KSI at different urea concentrations supported the two-state model without any evidence of folded monomeric intermediates. Consistent with the two-state model, (1)H-(15)N HSQC spectra obtained for KSI in the unfolding transition region could be reproduced by a simple addition of the spectra of the native and the unfolded KSI. The KSI refolding kinetics as monitored by fluorescence intensity could be described as a fast first-order process followed by a second-order and a subsequent slow first-order processes with rate constants of 60 s(-)(1), 5.4 x 10(4) M(-)(1).s(-)(1), and 0.017 s(-)(1), respectively, at 0.62 M urea, suggesting that there may be a monomeric folding intermediate. After a burst phase that accounts for >83% of the total amplitude, the negative molar ellipticity at 225 nm increased slowly in a single phase at a rate comparable to that of the bimolecular intermediate step. The kinetics of activity recovery from the denatured state were markedly dependent upon the protein concentration, implying that the monomers are not fully active. Taken together, our results demonstrate that the dimerization induces KSI to fold into the complete structure and is crucial for maintaining the tertiary structure to perform efficient catalysis.