Relationship between the native-state hydrogen exchange and folding pathways of a four-helix bundle protein

The hydrogen exchange behavior of a four-helix bundle protein in low concentrations of denaturant reveals some partially unfolded forms that are significantly more stable than the fully unfolded state. Kinetic folding of the protein, however, is apparently two-state in the absence of the accumulation of early folding intermediates. The partially unfolded forms are either as folded as or more folded than the rate-limiting transition state and appear to represent the major intermediates in a folding and unfolding reaction. These results are consistent with the suggestion that partially unfolded intermediates may form after the rate-limiting step for small proteins with apparent two-state folding kinetics.     

Molecular mechanism of the Zn2+-induced folding of the distal CCHC finger motif of the HIV-1 nucleocapsid protein

HIV-1 nucleocapsid protein, NCp7, contains two highly conserved CCHC zinc fingers. Binding of Zn(2+) drives NCp7 from an unfolded to a highly folded structure that is critical for its functions. Using the intrinsic fluorescence of Trp(37), we investigated, by the stopped-flow technique, the folding of NCp7 distal finger through the pH dependence of its Zn(2+) association and dissociation kinetics. Zn(2+) binding was found to involve four different paths associated with the four deprotonated states of the finger. Each binding path involves the rapid formation of an intermediate complex that is subsequently rearranged and stabilized in a rate-limiting step. The equilibrium and kinetic rate constants of the full Zn(2+)-binding process have been determined. At neutral pH, the preferential pathway for the Zn(2+)-driven folding implies Zn(2+) binding to the deprotonated Cys(36) and His(44) residues, in the bidentate state of the finger. The resulting intermediate is then converted with a rate constant of 500 s(-1) into a more suitably folded form, probably through a rearrangement of the peptide backbone around Zn(2+) to optimize the binding geometry. This form then rapidly leads to the final native complex, through deprotonation of Cys(39) and Cys(49) residues and intramolecular substitution of coordinated water molecules. Zn(2+) dissociation is also characterized by a multistep process and occurs fastest via the deprotonated Zn(2+)-bound bidentate state with a rate constant of 3 s(-1). Due to their critical role in folding, the intermediates identified for the first time in this study may constitute potential targets for HIV therapy.     

The "magic numbers" of metallothionein

Metallothioneins (MT) are a family of small cysteine rich proteins, which since their discovery in 1957, have been implicated in a range of roles including toxic metal detoxification, protection against oxidative stress, and as a metallochaperone involved in the homeostasis of both zinc and copper. The most well studied member of the family is the mammalian metallothionein, which consists of two domains: a β-domain with 9 cysteine residues, which sequesters 3 Cd(2+) or Zn(2+) or 6 Cu(+) ions, and an α-domain with 11 cysteine residues and, which sequesters 4 Cd(2+) or Zn(2+) or 6 Cu(+) ions. Despite over half a century of research, the exact functions of MT are still unknown. Much of current research aims to elucidate the mechanism of metal binding, as well as to isolate intermediates in metal exchange reactions; reactions necessary to maintain homeostatic equilibrium. These studies further our understanding of the role(s) of this remarkable and ubiquitous protein. Recently, supermetallated forms of the protein, where supermetallation describes metallation in excess of traditional levels, have been reported. These species may potentially be the metal exchange intermediates necessary to maintain homeostatic equilibrium. This review focuses on recent advances in the understanding of the mechanistic properties of metal binding, the implications for the metal induced protein folding reactions proposed for metallothionein metallation, the value of "magic numbers", which we informally define as the commonly determined metal-to-protein stoichiometric ratios and the significance of the new supermetallated states of the protein and the possible interpretation of the structural properties of this new metallation status. Together we provide a commentary on current experimental and theoretical advances and frame our consideration in terms of the possible functions of MT.     

A first-order-like state transition for recombinant protein folding

Normally, proteins will aggregate and precipitate by direct folding processes. In this study, we report that quasi-static processes can restore both the structure and bio-function of two kinds of fish recombinant growth hormones (Plecoglossus altivelis and Epinephelus awoara). The conformational changes and the particle-size-distribution (PSD) of each refolding intermediate can be monitored by circular dichroism spectroscopy (CD) and dynamic light scattering (DLS), respectively. Conformation analysis of the CD spectra of the refolding intermediates indicated that the secondary structures were restored in the initial refolding intermediate. However, the tertiary interactions of the proteins were restored during the last two refolding stages, as elucidated by thermal stability tests. This is consistent with a sequential model. DLS analysis suggested that the average hydrodynamic radii of the refolding intermediates shrank to their native-like sizes after the first refolding stage. This is consistent with a collapse model. After comparison with the data on the direct folding process, it is concluded that the denaturant-containing protein folding reaction is a first-order-like state transition process.     

Hidden intermediates and levinthal paradox in the folding of small proteins

It has long been suggested that existence of partially folded intermediates may be essential for proteins to fold in a biologically meaningful time scale. Although partially folded intermediates have been commonly observed in larger proteins, they are generally not detectable in the kinetic folding of smaller proteins (approximately 100 amino acids or less). Recent native-state hydrogen exchange studies suggest that partially folded intermediates may exist behind the rate-limiting transition state in small proteins and evade detection by conventional kinetic methods.     

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.     

Absence of a stable intermediate on the folding pathway of protein A.

The B-domain of protein A has one of the simplest protein topologies, a three-helix bundle. Its folding has been studied as a model for elementary steps in the folding of larger proteins. Earlier studies suggested that folding might occur by way of a helical hairpin intermediate. Equilibrium hydrogen exchange measurements indicate that the C-terminal helical hairpin could be a potential folding intermediate. Kinetic refolding experiments were performed using stopped-flow circular dichroism and NMR hydrogen-deuterium exchange pulse labeling. Folding of the entire molecule is essentially complete within the 6 ms dead time of the quench-flow apparatus, indicating that the intermediate, if formed, progresses rapidly to the final folded state. Site-directed mutagenesis of the isoleucine residue at position 16 was used to generate a variant protein containing tryptophan (the 116 W mutant). The formation of the putative folding intermediate was expected to be favored in this mutant at the expense of the native folded form, due to predicted unfavorable steric interactions of the bulky tryptophan side chain in the folded state. The 116 W mutant refolds completely within the dead time of a stopped-flow fluorescence experiment. No partly folded intermediate could be detected by either kinetic or equilibrium measurements. Studies of peptide fragments suggest that the protein A sequence has an intrinsic propensity to form a helix II/helix III hairpin. However, its stability appears to be marginal (of the order of 1/2 kT) and it could not be an obligatory intermediate on a defined folding pathway. These results explicitly demonstrate that the protein A B domain folds extremely rapidly by an apparent two-state mechanism without formation of stable partly folded intermediates. Similar mechanisms may also be involved in the rapid folding of subdomains of larger proteins to form the compact molten globule intermediates that often accumulate during the folding process.     

COSMIC analysis of the major alpha-helix of barnase during folding

The structures of transition states and intermediates in protein folding may be analysed by protein engineering methods that remove simple interactions that stabilize the folded state. We have now extended the range and reliability of the procedure by using the COSMIC (Combination of Sequential Mutant Interaction Cycles) technique, in which a series of double-mutant cycles is constructed. In each cycle, the side-chains of two amino acid residues that interact in the folded state are mutated separately and together. Kinetic and equilibrium measurements on folding for each cycle show unambiguously whether or not two residues interact during protein folding. A series of such cycles has been constructed to leapfrog along the major alpha-helix of barnase, comprising residues 6 to 18. The helix is found to be intact from its C terminus to residue 12 but begins to unwind towards the N terminus in both the transition state for unfolding and in a folding intermediate.     

The folding pathway of barnase: the rate-limiting transition state and a hidden intermediate under native conditions

The nature of the rate-limiting transition state at zero denaturant (TS(1)) and whether there are hidden intermediates are the two major unsolved problems in defining the folding pathway of barnase. In earlier studies, it was shown that TS(1) has small phi values throughout the structure of the protein, suggesting that the transition state has either a defined partially folded secondary structure with all side chains significantly exposed or numerous different partially unfolded structures with similar stability. To distinguish the two possibilities, we studied the effect of Gly mutations on the folding rate of barnase to investigate the secondary structure formation in the transition state. Two mutations in the same region of a beta-strand decreased the folding rate by 20- and 50-fold, respectively, suggesting that the secondary structures in this region are dominantly formed in the rate-limiting transition state. We also performed native-state hydrogen exchange experiments on barnase at pD 5.0 and 25 degrees C and identified a partially unfolded state. The structure of the intermediate was investigated using protein engineering and NMR. The results suggest that the intermediate has an omega loop unfolded. This intermediate is more folded than the rate-limiting transition state previously characterized at high denaturant concentrations (TS(2)). Therefore, it exists after TS(2) in folding. Consistent with this conclusion, the intermediate folds with the same rate and denaturant dependence as the wild-type protein, but unfolds faster with less dependence on the denaturant concentration. These and other results in the literature suggest that barnase folds through partially unfolded intermediates that exist after the rate-limiting step. Such folding behavior is similar to those of cytochrome c and Rd-apocyt b(562). Together, we suggest that other small apparently two-state proteins may also fold through hidden intermediates.     

The Folding Trajectory of RNase H Is Dominated by Its Topology and Not Local Stability: A Protein Engineering Study of Variants that Fold via Two-State and Three-State Mechanisms

Proteins can sample a variety of partially folded conformations during the transition between the unfolded and native states. Some proteins never significantly populate these high-energy states and fold by an apparently two-state process. However, many proteins populate detectable, partially folded forms during the folding process. The role of such intermediates is a matter of considerable debate. A single amino acid change can convert Escherichia coli ribonuclease H from a three-state folder that populates a kinetic intermediate to one that folds in an apparent two-state fashion. We have compared the folding trajectories of the three-state RNase H and the two-state RNase H, proteins with the same native-state topology but altered regional stability, using a protein engineering approach. Our data suggest that both versions of RNase H fold through a similar trajectory with similar high-energy conformations. Mutations in the core and the periphery of the protein affect similar aspects of folding for both variants, suggesting a common trajectory with folding of the core region followed by the folding of the periphery. Our results suggest that formation of specific partially folded conformations may be a general feature of protein folding that can promote, rather than hinder, efficient folding.     

Molecular basis of co-operativity in protein folding.

The folding/unfolding transition of proteins is a highly co-operative process characterized by the presence of very few or no thermodynamically stable partially folded intermediate states. The purpose of this paper is to present a thermodynamic formalism aimed at describing quantitatively the co-operative folding behavior of proteins. In order to account for this behavior, a hierarchical algorithm aimed at evaluating the folding/unfolding partition function has been developed. This formalism defines the partition function in terms of multiple levels of interacting co-operative folding units. A co-operative folding unit is defined as a protein structural element that exhibits two-state folding/unfolding behavior. At the most fundamental level are those structural elements that behave co-operatively as a result of purely local interactions. Higher-order co-operative folding units are formed through interactions between different structural elements. The hierarchical formalism utilizes the crystallographic structure of the protein as a template to generate partially folded conformations defined in terms of co-operative folding units. The Gibbs free energy of those states and their corresponding statistical weights are then computed using experimental energetic parameters determined calorimetrically. This formalism has been applied to the case of myoglobin. It is shown that the hierarchical partition function correctly predicts the presence, energetics and co-operativity of the heat and cold denaturation transitions. The major contribution to the co-operative folding behavior arises from the solvent exposure of non-polar residues located in regions complementary to those that have undergone unfolding. This entropically uncompensated and energetically unfavorable solvent exposure characterizes all partially folded states but not the unfolded state, thus minimizing the population of partially folded intermediates throughout the folding/unfolding transition.     

Disorder-to-order conformational transitions in protein structure and its relationship to disease

Function in proteins largely depends on the acquisition of specific structures through folding at physiological time scales. Under both equilibrium and non-equilibrium states, proteins develop partially structured molecules that being intermediates in the process, usually resemble the structure of the fully folded protein. These intermediates, known as molten globules, present the faculty of adopting a large variety of conformations mainly supported by changes in their side chains. Taking into account that the mechanism to obtain a fully packed structure is considered more difficult energetically than forming partially “disordered” folding intermediates, evolution might have conferred upon an important number of proteins the capability to first partially fold and—depending on the presence of specific partner ligands—switch on disorder-to-order transitions to adopt a highly ordered well-folded state and reach the lowest energy conformation possible. Disorder in this context can represent segments of proteins or complete proteins that might exist in the native state. Moreover, because this type of disorder-to-order transition in proteins has been found to be reversible, it has been frequently associated with important signaling events in the cell. Due to the central role of this phenomenon in cell biology, protein misfolding and aberrant disorder-to-order transitions have been at present associated with an important number of diseases.     

Noncooperative metalation of metallothionein 1a and its isolated domains with zinc

Mammalian metallothioneins (MTs) are a family of small cysteine-rich proteins capable of binding 7 Zn(2+) or Cd(2+) ions into two distinct domains: an N-terminal β-domain that binds 3 Zn(2+) or Cd(2+) and a C-terminal α-domain that binds 4 Zn(2+) or Cd(2+). MT has been implicated in a number of physiological functions, including metal ion homeostasis, toxic metal detoxification, and as a protective agent against oxidative stress. Conventionally, MT has been understood to coordinate metal ions in a cooperative fashion. Under this mechanism of metalation, the only species of biological relevance would be the metal-free (apo-) form of the protein and the fully metalated (holo-) form of the protein. However, an increasing body of evidence suggests that metalation occurs in a noncooperative manner. If this latter mechanism is correct, then partially metalated forms of the protein will be stable and able to take part in cellular chemistry. We report in this paper conclusive evidence that shows that biologically essential zinc binds to MT in a noncooperative manner. In addition, we report for the first time the stability of a Zn(5)-MT species. The implications of these findings are discussed in terms of the mechanism of metalation.     

Conformational detours during folding of a collapsed state

The protein S6 is a useful model to probe the role of partially folded states in the folding process. In the absence of salt, S6 folds from the denatured state D to the native state N without detectable intermediates. High concentrations of sodium sulfate induce the accumulation of a collapsed state C, which is off the direct folding route. However, the mutation VA85 enables S6 to fold from C directly to N through the transition state TS(C). According to the denaturant dependence of this reaction, TS(C) and C are equally compact, but the data are difficult to deconvolute. Therefore, I have measured the heat capacities (DeltaC(p)) for the D-->C and C-->TS(C) transitions. The DeltaC(p)-values suggest that C needs to increase its surface area in order to fold directly to N. This underlines that it is a misfolded state that can only fold by at least partial unfolding. In contrast to the C-state formed by S6 wildtype, the VA85 C-state is just as compact as the native state, and this may be a prerequisite for direct folding. Individual "gatekeeper" residues may thus play a disproportionately large role in guiding proteins through different folding pathways.     

Aggregation and assembly of phage P22 temperature-sensitive coat protein mutants in vitro mimic the in vivo phenotype

Aggregation is a common side reaction in the folding of proteins which is likely due to inappropriate interactions of folding intermediates. In the in vivo folding of phage P22 coat protein, amino acid substitutions that cause a temperature-sensitive-folding (tsf) phenotype lead to the localization of the mutant coat proteins to inclusion bodies. Investigated here is the aggregation of wild-type (WT) coat protein and 3 tsf mutants of coat protein. The tsf coat proteins aggregated when refolded in vitro at high temperature. If the tsf coat proteins were refolded at 4 degrees C, they were able attain an assembly active state. WT coat protein, on the other hand, did not aggregate significantly even when folded at high temperature. The refolded tsf mutants exhibited altered secondary and tertiary structures and had an increased surface hydrophobicity, which may explain the increased propensity of their folding intermediates to aggregate.     

Disulfide bonds and protein folding

The applications of disulfide-bond chemistry to studies of protein folding, structure, and stability are reviewed and illustrated with bovine pancreatic ribonuclease A (RNase A). After surveying the general properties and advantages of disulfide-bond studies, we illustrate the mechanism of reductive unfolding with RNase A, and discuss its application to probing structural fluctuations in folded proteins. The oxidative folding of RNase A is then described, focusing on the role of structure formation in the regeneration of the native disulfide bonds. The development of structure and conformational order in the disulfide intermediates during oxidative folding is characterized. Partially folded disulfide species are not observed, indicating that disulfide-coupled folding is highly cooperative. Contrary to the predictions of "rugged funnel" models of protein folding, misfolded disulfide species are also not observed despite the potentially stabilizing effect of many nonnative disulfide bonds. The mechanism of regenerating the native disulfide bonds suggests an analogous scenario for conformational folding. Finally, engineered covalent cross-links may be used to assay for the association of protein segments in the folding transition state, as illustrated with RNase A.     

Zn(2+)-dependent misfolding of the p53 DNA binding domain

The DNA binding domain (DBD) of p53 folds by a complex mechanism that involves parallel pathways and multiple intermediates, both on- and off-pathway. This heterogeneity renders DBD particularly susceptible to misfolding and aggregation. The origins of parallel folding mechanisms are not well understood. DBD folding heterogeneity may be caused by the presence of the single bound Zn2+. To test that hypothesis, we carried out kinetic folding studies of DBD in its Zn2+-free form (apoDBD) and in the presence of various concentrations of free Zn2+ and the Zn2+-nitrilotriacetate (NTA) complex. Folding kinetics of apoDBD and DBD are similar, although apoDBD folds faster than DBD at some urea concentrations. The principle consequence of Zn2+ removal is to accelerate unfolding and simplify it from two exponential phases to one. Metal binding interactions are therefore not responsible for the observed complexity of the folding reaction. A slight stoichiometric excess of free Zn2+ arrests folding and traps the protein in a misfolded state in which Zn2+ is bound to nonphysiological ligands. Folding can be rescued by providing metal ions in the form of the NTA-Zn2+ complex, which simultaneously protects against misligation and provides a source of Zn2+ for regenerating the functional protein. This chemical metallochaperone strategy may be an effective means for improving folding efficiency of other metal binding proteins. The findings suggest that, in vivo, DBD must fold in an environment where free Zn2+ concentration is low and its bioavailability is carefully regulated by cellular metallochaperones.     

Energetics of protein structure and folding

The available experimental date on the kinetics of unfolding and refolding of small proteins are reviewed. Excluding slow transitions in the unfolded protein due to cis–trans isomerization of peptide bonds, the rate-limiting transition state in both unfolding and refolding is concluded to be a high-energy distortion of the fully folded state. Partially folded intermediates are undoubtedly important for folding, but their formation is normally not rate limiting. A simple model is used to illustrate some of the aspects of protein-folding energetics.     

Energy barriers, cooperativity, and hidden intermediates in the folding of small proteins

Current theoretical views of the folding process of small proteins (< approximately 100 amino acids) postulate that the landscape of potential mean force (PMF) for the formation of the native state has a funnel shape and that the free energy barrier to folding arises from the chain configurational entropy only. However, recent theoretical studies on the formation of hydrophobic clusters with explicit water suggest that a barrier should exist on the PMF of folding, consistent with the fact that protein folding generally involves a large positive activation enthalpy at room temperature. In addition, high-resolution structural studies of the hidden partially unfolded intermediates have revealed the existence of non-native interactions, suggesting that the correction of the non-native interactions during folding should also lead to barriers on PMF. To explore the effect of a PMF barrier on the folding behavior of proteins, we modified Zwanzig's model for protein folding with an uphill landscape of PMF for the formation of transition states. We found that the modified model for short peptide segments can satisfy the thermodynamic and kinetic criteria for an apparently two-state folding. Since the Levinthal paradox can be solved by a stepwise folding of short peptide segments, a landscape of PMF with a locally uphill search for the transition state and cooperative stabilization of folding intermediates/native state is able to explain the available experimental results for small proteins. We speculate that the existence of cooperative hidden folding intermediates in small proteins could be the consequence of the highly specific structures of the native state, which are selected by evolution to perform specific functions and fold in a biologically meaningful time scale.