Stefano Gianni

Unifying features in protein-folding mechanisms

We compare the folding of representative members of a protein superfamily by experiment and simulation to investigate common features in folding mechanisms. The homeodomain superfamily of three-helical, single-domain proteins exhibits a spectrum of folding processes that spans the complete transition from concurrent secondary and tertiary structure formation (nucleation-condensation mechanism) to sequential secondary and tertiary formation (framework mechanism). The unifying factor in their mechanisms is that the transition state for (un)folding is expanded and very native-like, with the proportion and degree of formation of secondary and tertiary interactions varying. There is a transition, or slide, from the framework to nucleation-condensation mechanism with decreasing stability of the secondary structure. Thus, framework and nucleation-condensation are different manifestations of an underlying common mechanism.

Distinguishing induced fit from conformational selection

The interactions between proteins and ligands often involve a conformational change in the protein. This conformational change can occur before (conformational selection) or after (induced fit) the association with ligand. It is often very difficult to distinguish induced fit from conformational selection when hyperbolic binding kinetics are observed. In light of a recent paper in this journal (Vogt et al., Biophys. Chem., 186, 2014, 13-21) and the current interest in binding mechanisms emerging from observed sampling of distinct conformations in protein domains, as well as from the field of intrinsically disordered proteins, we here describe a kinetic method that, at least in some cases, unequivocally distinguishes induced fit from conformational selection. The method relies on measuring the observed rate constant λ for binding and varying both the protein and the ligand in separate experiments. Whereas induced fit always yields a hyperbolic dependence of increasing λ values, the conformational selection mechanism gives rise to distinct kinetics when the ligand and protein (displaying the conformational change) concentration is varied in separate experiments. We provide examples from the literature and discuss the limitations of the approach.

A PDZ domain recapitulates a unifying mechanism for protein folding

A unifying view has been recently proposed according to which the classical diffusion–collision and nucleation–condensation models may represent two extreme manifestations of an underlying common mechanism for the folding of small globular proteins. We report here the characterization of the folding process of the PDZ domain, a protein that recapitulates the three canonical steps involved in this unifying mechanism, namely: (i) the early formation of a weak nucleus that determines the native-like topology of a large portion of the structure, (ii) a global collapse of the entire polypeptide chain, and (iii) the consolidation of the remaining partially structured regions to achieve the native state conformation. These steps, which are clearly detectable in the PDZ domain investigated here, may be difficult to distinguish experimentally in other proteins, which would thus appear to follow one of the two limiting mechanisms. The analysis of the (un)folding kinetics for other three-state proteins (when available) appears consistent with the predictions ensuing from this unifying mechanism, thus providing a powerful validation of its general nature.

The binding mechanisms of intrinsically disordered proteins

Intrinsically disordered proteins (IDPs) and intrinsically disordered regions (IDRs) of proteins are very common and instrumental for cellular signaling. Recently, a number of studies have investigated the kinetic binding mechanisms of IDPs and IDRs. These results allow us to draw conclusions about the energy landscape for the coupled binding and folding of disordered proteins. The association rate constants of IDPs cover a wide range (10(5)-10(9) M(-1) s(-1)) and are largely governed by long-range charge-charge interactions, similarly to interactions between well-folded proteins. Off-rate constants also differ significantly among IDPs (with half-lives of up to several minutes) but are usually around 0.1-1000 s(-1), allowing for rapid dissociation of complexes. Likewise, affinities span from pM to μM suggesting that the low-affinity high-specificity concept for IDPs is not straightforward. Overall, it appears that binding precedes global folding although secondary structure elements such as helices may form before the protein-protein interaction. Short IDPs bind in apparent two-state reactions whereas larger IDPs often display complex multi-step binding reactions. While the two extreme cases of two-step binding (conformational selection and induced fit) or their combination into a square mechanism is an attractive model in theory, it is too simplistic in practice. Experiment and simulation suggest a more complex energy landscape in which IDPs bind targets through a combination of conformational selection before binding (e.g., secondary structure formation) and induced fit after binding (global folding and formation of short-range intermolecular interactions).

Parallel pathways in cytochrome c551 folding

The folding of cytochrome c(551) from Pseudomonas aeruginosa was previously thought to follow a simple sequential mechanism, consistent with the lack of histidine residues, other than the native His16 heme ligand, that can give rise to mis-coordinated species. However, further kinetic analysis reveals complexities indicative of a folding mechanism involving parallel pathways. Double-jump interrupted refolding experiments at low pH indicate that approximately 50% of the unfolded cytochrome c(551) population can reach the native state via a fast (10 ms) folding track, while the rest follows a slower folding path with populated intermediates. Stopped-flow experiments using absorbance at 695 nm to monitor refolding confirm the presence of a rapidly folding species containing the native methionine-iron bond while measurements on carboxymethylated cytochrome c(551) (which lacks the Met-Fe coordination bond) indicate that methionine ligation occurs late during folding along the fast folding track, which appears to be dominant at physiological pH. Continuous-flow measurements of tryptophan-heme energy transfer, using a capillary mixer with a dead time of about 60 micros, show evidence for a rapid chain collapse within 100 micros preceding the rate-limiting folding phase on the milliseconds time scale. A third process with a time constant in the 10-50 ms time range is consistent with a minor population of molecules folding along a parallel channel, as confirmed by quantitative kinetic modeling. These findings indicate the presence of two or more slowly inter-converting ensembles of denatured states that give rise to pH-dependent partitioning among fast and slow-folding pathways.

Structure of the transition state for the binding of c-Myb and KIX highlights an unexpected order for a disordered system

Significance A considerable fraction of proteins, although functional, does not display a well-ordered native state, posing the structure–function dogma into question. Although different models have been described, the role of protein disorder is still shrouded in mystery. Here, we investigate the mechanism of recognition between an intrinsically unstructured protein and its partner. Unexpectedly, we found the binding to occur with a very high degree of geometrical precision, suggesting that a potential value of disorder is not, in this case, to be searched in the speeding up of the reaction thanks to an increased capture radius. Given that in the cell disordered polypeptides may be more vulnerable than folded domains, the advantage in being natively unfolded remains a conundrum. A classical dogma of molecular biology dictates that the 3D structure of a protein is necessary for its function. However, a considerable fraction of the human proteome, although functional, does not adopt a defined folded state under physiological conditions. These intrinsically disordered proteins tend to fold upon binding to their partners with a molecular mechanism that is elusive to experimental characterization. Indeed, although many hypotheses have been put forward, the functional role (if any) of disorder in these intrinsically denatured systems is still shrouded in mystery. Here, we characterize the structure of the transition state of the binding-induced folding in the reaction between the KIX domain of the CREB-binding protein and the transactivation domain of c-Myb. The analysis, based on the characterization of a series of conservative site-directed mutants, reveals a very high content of native-like structure in the transition state and indicates that the recognition between KIX and c-Myb is geometrically precise. The implications of our results in the light of previous work on intrinsically unstructured systems are discussed.

Structural characterization of a misfolded intermediate populated during the folding process of a PDZ domain

Incorrectly folded states transiently populated during the protein folding process are potentially prone to aggregation and have been implicated in a range of misfolding disorders that include Alzheimers and Parkinsons diseases. Despite their importance, however, the structures of these states and the mechanism of their formation have largely escaped detailed characterization because of their short-lived nature. Here we present the structures of all the major states involved in the folding process of a PDZ domain, which include an off-pathway misfolded intermediate. By using a combination of kinetic, protein engineering, biophysical and computational techniques, we show that the misfolded intermediate is characterized by an alternative packing of the N-terminal β-hairpin onto an otherwise native-like scaffold. Our results suggest a mechanism of formation of incorrectly folded transient compact states by which misfolded structural elements are assembled together with more extended native-like regions.

Investigating the Structural Plasticity of a Cytochrome P450 THREE-DIMENSIONAL STRUCTURES OF P450 EryK AND BINDING TO ITS PHYSIOLOGICAL SUBSTRATE

Cytochrome P450s are heme-containing proteins that catalyze the oxidative metabolism of many physiological endogenous compounds. Because of their unique oxygen chemistry and their key role in drug and xenobiotic metabolism, particular attention has been devoted in elucidating their mechanism of substrate recognition. In this work, we analyzed the three-dimensional structures of a monomeric cytochrome P450 from Saccharopolyspora erythraea, commonly called EryK, and the binding kinetics to its physiological ligand, erythromycin D. Three different structures of EryK were obtained: two ligand-free forms and one in complex with its substrate. Analysis of the substrate-bound structure revealed the key structural determinants involved in substrate recognition and selectivity. Interestingly, the ligand-free structures of EryK suggested that the protein may explore an open and a closed conformation in the absence of substrate. In an effort to validate this hypothesis and to investigate the energetics between such alternative conformations, we performed stopped-flow absorbance experiments. Data demonstrated that EryK binds erythromycin D via a mechanism involving at least two steps. Contrary to previously characterized cytochrome P450s, analysis of double jump mixing experiments confirmed that this complex scenario arises from a pre-existing equilibrium between the open and closed subpopulations of EryK, rather than from an induced-fit type mechanism.

A sequential binding mechanism in a PDZ domain.

Conformational selection and induced fit are two well-known mechanisms of allosteric protein-ligand interaction. Some proteins, like ubiquitin, have recently been found to exist in multiple conformations at equilibrium, suggesting that the conformational selection may be a general mechanism of interaction, in particular for single-domain proteins. Here, we found that the PDZ2 domain of SAP97 binds its ligand via a sequential (induced fit) mechanism. We performed binding experiments using SAP97 PDZ2 and peptide ligands and observed biphasic kinetics with the stopped-flow technique, indicating that ligand binding involves at least a two-step process. By using an ultrarapid continuous-flow mixer, we then detected a hyperbolic dependence of binding rate constants on peptide concentration, corroborating the two-step binding mechanism. Furthermore, we found a similar dependence of the rate constants on both PDZ and peptide concentration, demonstrating that the PDZ2-peptide interaction involves a precomplex, which then undergoes a conformational change, and thereby follows an induced fit mechanism.

A folding-after-binding mechanism describes the recognition between the transactivation domain of c-Myb and the KIX domain of the CREB-binding protein

A large body of evidence suggests that a considerable fraction of the human proteome may be at least in part intrinsically unstructured. While disordered, intrinsically unstructured proteins are nevertheless functional and mediate many interactions. Despite their significant role in regulation, however, little is known about the molecular mechanism whereby intrinsically unstructured proteins exert their function. This basic problem is critical to establish the role, if any, of disorder in cellular systems. Here we present kinetic experiments supporting a mechanism of binding-induced-folding when the KIX domain of the CREB-binding protein binds the transactivation domain of c-Myb, an intrinsically unstructured domain. The high-resolution structure of this physiologically important complex was previously determined by NMR spectroscopy. Our data reveal that c-Myb recognizes KIX by first forming a weak encounter complex in a disordered conformation, which is subsequently locked-in by a folding step, i.e. binding precedes folding. On the basis of the pH dependence of the observed combination and dissociation rate constants we propose a plausible mechanism for complex formation. The implications of our results in the light of previous work on intrinsically unstructured systems are discussed.