In vitro evolution of a hyperstable Gbeta1 variant

An in-vitro selection strategy was used to obtain strongly stabilized variants of the beta1 domain of protein G (Gbeta1). In a two-step approach, first candidate positions with a high potential for stabilization were identified in Gbeta1 libraries that were created by error-prone PCR, and then, after randomization of these positions by saturation mutagenesis, strongly stabilized variants were selected. For both steps the in-vitro selection method Proside was employed. Proside links the stability of a protein with the infectivity of a filamentous phage. Ultimately, residues from the two best selected variants were combined in a single Gbeta1 molecule. This variant with the four mutations E15V, T16L, T18I, and N37L showed an increase of 35.1 degrees C in the transition midpoint and of 28.5 kJ mol(-1) (at 70 degrees C) in the Gibbs free energy of stabilization. It was considerably more stable than the best variant from a previous Proside selection, in which positions were randomized that had originally been identified by computational design. Only a single substitution (T18I) was found in both selections. The best variants from the present selection showed a higher cooperativity of thermal unfolding, as indicated by an increase in the enthalpy of unfolding by about 60 kJ mol(-1). This increase is apparently correlated with the presence of Leu residues that were selected at the positions 16 and 37.     

Desolvation and Development of Specific Hydrophobic Core Packing during Im7 Folding

Development of a tightly packed hydrophobic core drives the folding of water-soluble globular proteins and is a key determinant of protein stability. Despite this, there remains much to be learnt about how and when the hydrophobic core becomes desolvated and tightly packed during protein folding. We have used the bacterial immunity protein Im7 to examine the specificity of hydrophobic core packing during folding. This small, four-helix protein has previously been shown to fold via a compact three-helical intermediate state. Here, overpacking substitutions, in which residue side-chain size is increased, were used to examine the specificity and malleability of core packing in the folding intermediate and rate-limiting transition state. In parallel, polar groups were introduced into the Im7 hydrophobic core via Val→Thr or Phe→Tyr substitutions and used to determine the solvation status of core residues at different stages of folding. Over 30 Im7 variants were created allowing both series of substitutions to cover all regions of the protein structure. Φ-value analysis demonstrated that the major changes in Im7 core solvation occur prior to the population of the folding intermediate, with key regions involved in docking of the short helix III remaining solvent-exposed until after the rate-limiting transition state has been traversed. In contrast, overpacking core residues revealed that some regions of the native Im7 core are remarkably malleable to increases in side-chain volume. Overpacking residues in other regions of the Im7 core result in substantial (> 2.5 kJ mol^− 1) destabilisation of the native structure or even prevents efficient folding to the native state. This study provides new insights into Im7 folding; demonstrating that whilst desolvation occurs early during folding, adoption of a specifically packed core is achieved only at the very last step in the folding mechanism.     

Structural comparison of the two alternative transition states for folding of TI I27

TI I27, a beta-sandwich domain from the human muscle protein titin, has been shown to fold via two alternative pathways, which correspond to a change in the folding mechanism. Under physiological conditions, TI I27 folds by a classical nucleation-condensation mechanism (diffuse transition state), whereas at extreme conditions of temperature and denaturant it switches to having a polarized transition state. We have used experimental Phi-values as restraints in ensemble-averaged molecular dynamics simulations to determine the ensembles of structures representing the two transition states. The comparison of these ensembles indicates that when native interactions are substantially weakened, a protein may still be able to fold if it can access an alternative transition state characterized by a much larger entropic contribution. Analysis of the probability distribution of Phi-values derived from ensemble averaged simulations, enables us to identify residues that form contacts in some members of the ensemble but not in others illustrating that many interactions present in transition states are not strictly required for the successful completion of the folding process.     

Specificity of the initial collapse in the folding of the cold shock protein

The two-state folding reaction of the cold shock protein from Bacillus caldolyticus (Bc-Csp) is preceded by a rapid chain collapse. A fast shortening of intra-protein distances was revealed by F?rster resonance energy transfer (FRET) measurements with protein variants that carried individual pairs of donor and acceptor chromophores at various positions along the polypeptide chain. Here we investigated the specificity of this rapid compaction. Energy transfer experiments that probed the stretching of strand beta2 and the close approach between the strands beta1 and beta2 revealed that the beta1-beta2 hairpin is barely formed in the collapsed form, although it is native-like in the folding transition state of Bc-Csp. The time course of the collapse could not be resolved by pressure or temperature jump experiments, indicating that the collapsed and extended forms are not separated by an energy barrier. The co-solute (NH4)2SO4 stabilizes both native Bc-Csp and the collapsed form, which suggests that the large hydrated SO4(2-) ions are excluded from the surface of the collapsed form in a similar fashion as they are excluded from folded Bc-Csp. Ethylene glycol increases the stability of proteins because it is excluded preferentially from the backbone, which is accessible in the unfolded state. The collapsed form of Bc-Csp resembles the unfolded form in its interaction with ethylene glycol, suggesting that in the collapsed form the backbone is still accessible to water and small molecules. Our results thus rule out that the collapsed form is a folding intermediate with native-like chain topology. It is better described as a mixture of compact conformations that belong to the unfolded state ensemble. However, some of its structural elements are reminiscent of the native protein.     

Energetic coupling between native-state prolyl isomerization and conformational protein folding

In folded proteins, prolyl peptide bonds are usually thought to be either trans or cis because only one of the isomers can be accommodated in the native folded protein. For the N-terminal domain of the gene-3 protein of the filamentous phage fd (N2 domain), Pro161 resides at the tip of a beta hairpin and was found to be cis in the crystal structure of this protein. Here we show that Pro161 exists in both the cis and the trans conformations in the folded form of the N2 domain. We investigated how conformational folding and prolyl isomerization are coupled in the unfolding and refolding of N2 domain. A combination of single-mixing and double-mixing unfolding and refolding experiments showed that, in unfolded N2 domain, 7% of the molecules contain a cis-Pro161 and 93% of the molecules contain a trans-Pro161. During refolding, the fraction of molecules with a cis-Pro161 increases to 85%. This implies that 10.3 kJ mol(-1) of the folding free energy was used to drive this 75-fold change in the Pro161 cis/trans equilibrium constant during folding. The stabilities of the forms with the cis and the trans isomers of Pro161 and their folding kinetics could be determined separately because their conformational folding is much faster than the prolyl isomerization reactions in the native and the unfolded proteins. The energetic coupling between conformational folding and Pro161 isomerization is already fully established in the transition state of folding, and the two isomeric forms are thus truly native forms. The folding kinetics are well described by a four-species box model, in which the N2 molecules with either isomer of Pro161 can fold to the native state and in which cis/trans isomerization occurs in both the unfolded and the folded proteins.     

Kinetic isotope effects reveal the presence of significant secondary structure in the transition state for the folding of the N-terminal domain of L9

Our present understanding of the nature of the transition state for protein folding depends predominantly on studies where individual side-chain contributions are mapped out by mutational analysis (phi value analysis). This approach, although extremely powerful, does not in general provide direct information about the formation of backbone hydrogen bonds. Here, we report the results of amide H/D isotope effect studies that probe the development of hydrogen bonded interactions in the transition state for the folding of a small alpha-beta protein, the N-terminal domain of L9. Replacement of amide protons by deuterons in a solvent of constant isotopic composition destabilized the domain, decreasing both its T(m) and Delta G(0) of unfolding. The folding rate also decreased. The parameter Phi(H/D), defined as the ratio of the effect of isotopic substitution upon the activation free energy to the equilibrium free energy was determined to be 0.6 in a D(2)O background and 0.75 in a H(2)O background, indicating that significant intraprotein hydrogen bond interactions are developed in the transition state for the folding of NTL9. The value is in remarkably good agreement with more traditional measures of the position of the transition state, which report on the relative burial of surface area. The results provide a picture of a compact folding transition state containing significant secondary structure. Indirect analysis argues that the bulk of the kinetic isotope effect arises from the beta-sheet-rich region of the protein, and suggests that the development of intraprotein hydrogen bonds in this region plays a critical role in the folding of NTL9.     

Molecular Determinants of a Native-State Prolyl Isomerization

Prolyl cis/trans isomerizations determine the rates of many protein-folding reactions, and they can serve as molecular switches and timers. The energy required to shift the prolyl cis/trans equilibrium during these processes originates from conformational reactions that are linked structurally and energetically with prolyl isomerization. We used the N2 domain of the gene-3-protein of phage fd to elucidate how such an energetic linkage develops in the course of folding. The Asp160-Pro161 bond at the tip of a β hairpin of N2 is cis in the crystal structure, but in fact, it exists as a mixture of conformers in folded N2. During refolding, about 10 kJ mol^− 1 of conformational energy becomes available for a 75-fold shift of the cis/trans equilibrium constant at Pro161, from 7/93 in the unfolded to 90/10 in the folded form. We combined single- and double-mixing kinetic experiments with a mutational analysis to identify the structural origin of this proline shift energy and to elucidate the molecular path for the transfer of this energy to Pro161. It originates largely, if not entirely, from the two-stranded β sheet at the base of the Pro161 hairpin. The two strands improve their stabilizing interactions when Pro161 is cis, and this stabilization is propagated to Pro161, because the connector peptides between the β strands and Pro161 are native-like folded when Pro161 is cis. In the presence of a trans-Pro161, the connector peptides are locally unfolded, and thus, Pro161 is structurally and energetically uncoupled from the β sheet. Such interrelations between local folding and prolyl isomerization and the potential modulation by prolyl isomerases might also be used to break and reestablish slow communication pathways in proteins.     

Effects of heme on the structure of the denatured state and folding kinetics of cytochrome b562

Heme-linked proteins, such as cytochromes, are popular subjects for protein folding studies. There is the underlying question of whether the heme affects the structure of the denatured state by cross-linking it and forming other interactions, which would perturb the folding pathway. We have studied wild-type and mutant cytochrome b562 from Escherichia coli, a 106 residue four-alpha-helical bundle. The holo protein apparently refolds with a half-life of 4 micros in its ferrous state. We have analysed the folding of the apo protein using continuous-flow fluorescence as well as stopped-flow fluorescence and CD. The apo protein folded much more slowly with a half-life of 270 micros that was unaffected by the presence of exogenous heme. We examined the nature of the denatured states of both holo and apo proteins by NMR methods over a range of concentrations of guanidine hydrochloride. The starting point for folding of the holo protein in concentrations of denaturant around the denaturation transition was a highly ordered native-like species with heme bound. Fully denatured holo protein at higher concentrations of denaturant consisted of denatured apo protein and free heme. Our results suggest that the very fast folding species of denatured holo protein is in a compact state, whereas the normal folding pathway from fully denatured holo protein consists of the slower folding of the apo protein followed by the binding of heme. These data should be considered in the analysis of folding of heme proteins.     

The high-resolution NMR structure of the early folding intermediate of the Thermus thermophilus ribonuclease H

Elucidation of the high-resolution structures of folding intermediates is a necessary but difficult step toward the ultimate understanding of the mechanism of protein folding. Here, using hydrogen-exchange-directed protein engineering, we populated the folding intermediate of the Thermus thermophilus ribonuclease H, which forms before the rate-limiting transition state, by removing the unfolded regions of the intermediate, including an α-helix and two β-strands (51 folded residues). Using multidimensional NMR, we solved the structure of this intermediate mimic to an atomic resolution (backbone rmsd, 0.51 Å). It has a native-like backbone topology and shows some local deviations from the native structure, revealing that the structure of the folded region of an early folding intermediate can be as well defined as the native structure. The topological parameters calculated from the structures of the intermediate mimic and the native state predict that the intermediate should fold on a millisecond time scale or less and form much faster than the native state. Other factors that may lead to the slow folding of the native state and the accumulation of the intermediate before the rate-limiting transition state are also discussed.     

Searching for multiple folding pathways of a nearly symmetrical protein: temperature dependent phi-value analysis of the B domain of protein A

The B domain of protein A (BdpA) is a popular paradigm for simulating protein folding pathways. The discrepancies between so many simulations and subsequent experimental testing may be attributable to the protein being highly symmetrical: changing experimental conditions could perturb the subtle interplay between the effects of symmetry in the native structure and the effects of asymmetry from specific interactions in a given sequence. If the protein folds via multiple pathways, perturbations, such as temperature, denaturant concentration, and mutation, should change the flux of micro pathways, leading to changes in the bulk properties of the transition state. We tested this hypothesis by conducting a Phi-analysis of BdpA as a function of temperature from 25.0 degrees C to 60.0 degrees C. The Phi-values had no significant dependence on temperature and the values at 55.0 degrees C (denaturing conditions) are very similar to those at 25.0 degrees C (folding conditions), indicating the structure of the transition state does not significantly change although the experimental conditions are considerably altered. The results suggest that BdpA folds via a single dominant folding pathway.     

Optimized variants of the cold shock protein from in vitro selection: structural basis of their high thermostability

The bacterial cold shock proteins (Csp) are widely used as models for the experimental and computational analysis of protein stability. In a previous study, in vitro evolution was employed to identify strongly stabilizing mutations in Bs-CspB from Bacillus subtilis. The best variant found by this approach contained the mutations M1R, E3K and K65I, which raised the midpoint of thermal unfolding of Bs-CspB from 53.8 degrees C to 83.7 degrees C, and increased the Gibbs free energy of stabilization by 20.9 kJ mol(-1). Another selected variant with the two mutations A46K and S48R was stabilized by 11.1 kJ mol(-1). To elucidate the molecular basis of these stabilizations, we determined the crystal structures of these two Bs-CspB variants. The mutated residues are generally well ordered and provide additional stabilizing interactions, such as charge interactions, additional hydrogen bonds and improved side-chain packing. Several mutations improve the electrostatic interactions, either by the removal of unfavorable charges (E3K) or by compensating their destabilizing interactions (A46K, S48R). The stabilizing mutations are clustered at a contiguous surface area of Bs-CspB, which apparently is critically important for the stability of the beta-barrel structure but not well optimized in the wild-type protein.     

Electrostatic interactions in the denatured state and in the transition state for protein folding: effects of denatured state interactions on the analysis of transition state structure

The development of electrostatic interactions during the folding of the N-terminal domain of the ribosomal protein L9 (NTL9) is investigated by pH-dependent rate equilibrium free energy relationships. We show that Asp8, among six acidic residues, is involved in non-native, electrostatic interactions with K12 in the transition state for folding as well as in the denatured state. The perturbed native state pK(a) of D8 (pK(a) = 3.0) appears to be maintained through non-native interactions in both the transition state and the denatured state. Mutational effects on the stability of the transition state for protein (un)folding are often analyzed in respect to change in ground states. Thus, the interpretation of transition state analysis critically depends on an understanding of mutational effects on both the native and denatured state. Increasing evidence for structurally biased denatured states under physiological conditions raises concerns about possible denatured state effects on folding studies. We show that the structural interpretation of transition state analysis can be altered dramatically by denatured state effects.     

Correspondence between anomalous m- and DeltaCp-values in protein folding

Proteins folding according to a classical two-state system characteristically show V-shaped chevron plots. We have previously interpreted the symmetrically curved chevron plot of the protein U1A as denaturant-dependent movements in the position of the transition state ensemble (TSE). S6, a structural analog of U1A, shows a classical V-shaped chevron plot indicative of straightforward two-state kinetics, but the mutant LA30 has a curved unfolding limb, which is most consistent with TSE mobility. The kinetic m-values (derivatives of the rate constants with respect to denaturant concentration) in themselves depend on denaturant concentration. To obtain complementary information about putative mobile TSEs, we have carried out a thermodynamic analysis of the three proteins, based on data for refolding and unfolding over the range 10 degrees C to 70 degrees C. The data at all temperatures can be fitted to two-state model systems. Importantly, for all three proteins the activation heat capacities are, within error, identical to the heat capacities measured in independent experiments under equilibrium conditions. Although the equilibrium heat capacities are essentially invariant with regard to denaturant concentration, the activation heat capacities, similar to the structurally equivalent kinetic m-values, show marked denaturant dependence. Furthermore, the values of beta++ at different denaturant concentrations measured by m-values and by heat capacity values are very similar. These observations are consistent with significant transition state movements within the framework of two-state folding. The basis for TSE movement appears to be enthalpic rather than entropic, suggesting that the binding energy of denaturant-protein interactions is a major determinant of the response of energy landscape contours to changing environments.     

The cold denatured state is compact but expands at low temperatures: hydrodynamic properties of the cold denatured state of the C-terminal domain of L9

A point mutation of a small globular protein, the C-terminal domain of L9 destabilizes the protein and leads to observable cold-denaturation at temperatures above zero. The cold denatured state is in slow exchange with the native state on the NMR time scale, and this allows the hydrodynamic properties of the cold unfolded state and the native state to be measured under identical conditions using pulsed-field gradient NMR diffusion measurements. This provides the first experimental measurement of the hydrodynamic properties of a cold unfolded protein and its folded form under identical conditions. Hydrodynamic radii of the cold-induced unfolded states were measured for a set of temperatures ranging from 2 °C to 25 °C at pD 6.6 in the absence of denaturant. The cold unfolded state is compact compared to the urea or acid unfolded state and a trend of increasing radii of hydration is observed as the temperature is lowered. These observations are confirmed by experiments on the same protein at pD 8.0, where it is more stable, in the presence of a modest concentration of urea. The expansion of the cold-denatured state at lower temperatures is consistent with the temperature dependence of hydrophobic interactions.     

Consequences of Domain Insertion on the Stability and Folding Mechanism of a Protein

SlyD, the sensitive-to-lysis protein from Escherichia coli, consists of two domains. They are not arranged successively along the protein chain, but one domain, the “insert-in-flap” (IF) domain, is inserted internally as a guest into a surface loop of the host domain, which is a prolyl isomerase of the FK506 binding protein (FKBP) type. We used SlyD as a model to elucidate how such a domain insertion affects the stability and folding mechanism of the host and the guest domain. For these studies, the two-domain protein was compared with a single-domain variant SlyDΔIF, SlyD* without the chaperone domain (residues 1-69 and 130-165) in which the IF domain was removed and replaced by a short loop, as present in human FKBP12. Equilibrium unfolding and folding kinetics followed an apparent two-state mechanism in the absence and in the presence of the IF domain. The inserted domain decreased, however, the stability of the host domain in the transition region and decelerated its refolding reaction by about 10-fold. This originates from the interruption of the chain connectivity by the IF domain and its inherent instability. To monitor folding processes in this domain selectively, a Trp residue was introduced as fluorescent probe. Kinetic double-mixing experiments revealed that, in intact SlyD, the IF domain folds and unfolds about 1000-fold more rapidly than the FKBP domain, and that it is strongly stabilized when linked with the folded FKBP domain. The unfolding limbs of the kinetic chevrons of SlyD show a strong downward curvature. This deviation from linearity is not caused by a transition-state movement, as often assumed, but by the accumulation of a silent unfolding intermediate at high denaturant concentrations. In this kinetic intermediate, the FKBP domain is still folded, whereas the IF domain is already unfolded.     

The unfolded state of the villin headpiece helical subdomain: computational studies of the role of locally stabilized structure

The 36 residue villin headpiece helical subdomain (HP36) is one of the fastest cooperatively folding proteins, folding on the microsecond timescale. HP36's simple three helix topology, fast folding and small size have made it an attractive model system for computational and experimental studies of protein folding. Recent experimental studies have explored the denatured state of HP36 using fragment analysis coupled with relatively low-resolution spectroscopic techniques. These studies have shown that there is apparently only a small tendency to form locally stabilized secondary structure. Here, we complement the experimental studies by using replica exchange molecular dynamics with explicit solvent to investigate the structural features of these peptide models of unfolded HP36. To ensure convergence, two sets of simulations for each fragment were performed with different initial structures, and simulations were continued until these generated very similar final ensembles. These simulations reveal low populations of native-like structure and early folding events that cannot be resolved by experiment. For each fragment, calculated J-coupling constants and helical propensities are in good agreement with experimental trends. HP-1, corresponding to residues 41 to 53 and including the first alpha-helix, contains the highest helical population. HP-3, corresponding to residues 62 through 75 and including the third alpha-helix, contains a small population of helical turn residing at the N terminus while HP-2, corresponding to residues 52 through 61 and including the second alpha-helix, formed little to no structure in isolation. Overall, HP-1 was the only fragment to adopt a native-like conformation, but the low population suggests that formation of significant structure only occurs after formation of specific tertiary interactions.     

Phi-analysis of the folding of the B domain of protein A using multiple optical probes

We examined the co-operativity of ultra-fast folding of a protein and whether the Phi-value analysis of its transition state depended on the location of the optical probe. We incorporated in turn a tryptophan residue into each of the three helices of the B domain of Protein A. Each Trp mutant of the three-helix bundle protein was used as a pseudo-wild-type parent for Phi-analysis in which the intrinsic Trp fluorescence probed the formation of each helix during the transition state. Apart from local effects in the immediate vicinity of the probe, the three separate sets of Phi-values were in excellent agreement, demonstrating the overall co-operativity of folding and the robustness of the Phi-analysis. The transition state of folding of Protein A contains the second helix being well formed with many stabilizing tertiary hydrophobic interactions. In contrast, the first and the third helices are more poorly structured in the transition state. The mechanism of folding thus involves the concurrent formation of secondary and tertiary interactions, and is towards the nucleation-condensation extreme in the nucleation-condensation-framework continuum of mechanism, with helix 2 being the nucleus. We provide an error analysis of Phi-values derived purely from the kinetics of two-state chevron plots.     

Origins of the high stability of an in vitro-selected cold-shock protein

In previous work, we had identified stabilized forms of the cold-shock protein Bs-CspB from Bacillus subtilis in a combinatorial library by an in vitro selection procedure. In this library, the sequence positions 2, 3, 46, 64, 66, and 67 had been randomized, because Bs-CspB differs from the naturally thermostable homolog Bc-Csp from Bacillus caldolyticus, among others, at these six positions. For the most stable selected variant, the midpoint of thermal unfolding (tM) increased by 28.2 deg. C and the Gibbs free energy of unfolding (deltaG(D)) by 19 kJ/mol. Here, we analyzed by site-directed mutagenesis how the selected residues contribute individually to this strong stabilization. Val3 and Val66, which replace Glu3 and Glu66 of wild-type Bs-CspB, each contribute about 7 kJ/mol to stability, the Thr64Arg substitution contributes 4.5 kJ/mol, and 3.2 kJ/mol originate from the Ala46Leu replacement. Gly67 at the carboxy terminus is unimportant for stability, the Arg selected at position 2 is overall slightly destabilizing but improves the coulombic interactions. The best variant differs from Bc-Csp at all six positions; nevertheless, natural and in vitro selection followed similar principles. In both cases, negatively charged residues at the adjacent positions 3 and 66 are avoided, and a positively charged residue is introduced into this area of the protein surface. Its exact location is unimportant. It can be at position 3, as in the thermophilic Bc-Csp, or at positions 2 or 64, as in the most stable selected variant. These positively charged residues contribute to stability not by engaging in pairwise coulombic interactions with a specific carboxyl group, but by generally improving the charge distribution in this particular region of the protein surface. These coulombic effects contribute significantly to the thermostability of the cold-shock proteins. They are only weakly interdependent and best explained by the presence of a flexible ion network at the protein surface. Our results emphasize that surface positions are very good candidates for optimizing protein stability.     

Amino Acid Insertion Reveals a Necessary Three-Helical Intermediate in the Folding Pathway of the Colicin E7 Immunity Protein Im7

The small (87-residue) α-helical protein Im7 (an inhibitor protein for colicin E7 that provides immunity to cells producing colicin E7) folds via a three-state mechanism involving an on-pathway intermediate. This kinetic intermediate contains three of four native helices that are oriented in a non-native manner so as to minimise exposed hydrophobic surface area at this point in folding. The short (6-residue) helix III has been shown to be unstructured in the intermediate ensemble and does not dock onto the developing hydrophobic core until after the rate-limiting transition state has been traversed. After helix III has docked, it adopts an α-helical secondary structure, and the side chains of residues within this region provide contacts that are crucial to native-state stability. In order to probe further the role of helix III in the folding mechanism of Im7, we created a variant that contains an eight-amino-acid polyalanine-like helix stabilised by a Glu-Arg salt bridge and an Asn-Pro-Gly capping motif, juxtaposed C-terminal to the natural 6-residue helix III. The effect of this insertion on the structure of the native protein and its folding mechanism were studied using NMR and ?-value analysis, respectively. The results reveal a robust native structure that is not perturbed by the presence of the extended helix III. Mutational analysis performed to probe the folding mechanism of the redesigned protein revealed a conserved mechanism involving the canonical three-helical intermediate. The results suggest that folding via a three-helical species stabilised by both native and non-native interactions is an essential feature of Im7 folding, independent of the helical propensity of helix III.     

Probing the influence on folding behavior of structurally conserved core residues in P. aeruginosa apo-azurin

The effects on folding kinetics and equilibrium stability of core mutations in the apo-mutant C112S of azurin from Pseudomonas aeruginosa were studied. A number of conserved residues within the cupredoxin family were recognized by sequential alignment as constituting a common hydrophobic core: I7, F15, L33, W48, F110, L50, V95, and V31. Of these, I7, V31, L33, and L50 were mutated for the purpose of obtaining information on the transition state and a potential folding nucleus. In addition, residue V5 in the immediate vicinity of the common core, as well as T52, separate from the core, were mutated as controls. All mutants exhibited a nonlinear dependence of activation free energy of folding on denaturant concentration, although the refolding kinetics of the V31A/C112S mutant indicated that the V31A mutation destabilizes the transition state enough to allow folding via a parallel transition state ensemble. Phi-values could be calculated for three of the six mutants, V31A/C112S, L33A/C112S, and L50A/C112S, and the fractional values of 0.63, 0.33, and 0.50 (respectively) obtained at 0.5 M GdmCl suggest that these residues are important for stabilizing the transition state. Furthermore, a linear dependence of ln k(obs)(H2O) on DeltaG(U-N)(H2O) of the core mutations and the putative involvement of ground-state effects suggest the presence of native-like residual interactions in the denatured state that bias this ensemble toward a folding-competent state.