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.kinetics | mutagenesis | protein folding
In the past decade, a wealth of experimental data has demonstrated that a large fraction of proteins, while functional, are intrinsically disordered at physiological conditions. Many intrinsically disordered proteins (IDPs) undergo a disorder-to-order transition upon binding to their biological targets, a phenomenon known as induced folding. Induced folding may occur through two extreme mechanisms, namely conformational selection and folding after binding. Although the pre-existence of ordered structures in IDPs is a prerequisite for conformational selection, it does not necessarily commit to this latter mechanism, and kinetic studies are needed to discriminate between the two possible scenarios. So far, relatively few studies have addressed this issue from an experimental perspective. Here, we analyze the interaction kinetics between the intrinsically disordered C-terminal domain of the measles virus nucleoprotein (NTAIL) and the X domain (XD) of the viral phosphoprotein. Data reveal that NTAIL recognizes XD 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. The implications of our kinetic results, in the context of previously reported equilibrium data, are discussed. These results contribute to enhancing our understanding of the molecular mechanisms by which IDPs recognize their partners and represent a paradigmatic example of the need of kinetic methods to discriminate between reaction mechanisms.
The hydrophobic effect is a major driving force in protein folding. A complete understanding of this effect requires the description of the conformational states of water and protein molecules at different temperatures. Towards this goal, we characterise the cold and hot denatured states of a protein by modelling NMR chemical shifts using restrained molecular dynamics simulations. A detailed analysis of the resulting structures reveals that water molecules in the bulk and at the protein interface form on average the same number of hydrogen bonds. Thus, even if proteins are ‘large’ particles (in terms of the hydrophobic effect, i.e. larger than 1 nm), because of the presence of complex surface patterns of polar and non-polar residues their behaviour can be compared to that of ‘small’ particles (i.e. smaller than 1 nm). We thus find that the hot denatured state is more compact and richer in secondary structure than the cold denatured state, since water at lower temperatures can form more hydrogen bonds than at high temperatures. Then, using Φ-value analysis we show that the structural differences between the hot and cold denatured states result in two alternative folding mechanisms. These findings thus illustrate how the analysis of water-protein hydrogen bonds can reveal the molecular origins of protein behaviours associated with the hydrophobic effect.
The protein folding problem is often studied by comparing the mechanisms of proteins sharing the same structure but different sequence. The recent design of the two proteins G A 88 and G B 88, displaying different structures and functions while sharing 88% sequence identity (49 out of 56 amino acids), allows the unique opportunity for a complementary approach. At which stage of its folding pathway does a protein commit to a given topology? Which residues are crucial in directing folding mechanisms to a given structure? By using a combination of biophysical and computational techniques, we have characterized the folding of both G A 88 and G B 88. We show that, contrary to expectation, G B 88, characterized by a native ␣؉ fold, displays in the denatured state a content of native-like helical structure greater than G A 88, which is all-␣ in its native state. Both experiments and simulations indicate that such residual structure may be tuned by changing pH. Thus, despite the high sequence identity, the folding pathways for these two proteins appear to diverge as early as in the denatured state. Our results suggest a mechanism whereby protein topology is committed very early along the folding pathway, being imprinted in the residual structure of the denatured state.
Folding and function may impose different requirements on the amino acid sequences of proteins, thus potentially giving rise to conflict. Such a conflict, or frustration, can result in the formation of partially misfolded intermediates that can compromise folding and promote aggregation. We investigate this phenomenon by studying frataxin, a protein whose normal function is to facilitate the formation of iron-sulfur clusters but whose mutations are associated with Friedreich's ataxia. To characterize the folding pathway of this protein we carry out a Φ-value analysis and use the resulting structural information to determine the structure of the folding transition state, which we then validate by a second round of rationally designed mutagenesis. The analysis of the transition-state structure reveals that the regions involved in the folding process are highly aggregation-prone. By contrast, the regions that are functionally important are partially misfolded in the transition state but highly resistant to aggregation. Taken together, these results indicate that in frataxin the competition between folding and function creates the possibility of misfolding, and that to prevent aggregation the amino acid sequence of this protein is optimized to be highly resistant to aggregation in the regions involved in misfolding.
The folding pathway of the small α/β protein GB1 has been extensively studied during the past two decades using both theoretical and experimental approaches. These studies provided a consensus view that the protein folds in a two-state manner. Here, we reassessed the folding of GB1, both by experiments and simulations, and detected the presence of an on-pathway intermediate. This intermediate has eluded earlier experimental characterization and is distinct from the collapsed state previously identified using ultrarapid mixing. Failure to identify the presence of an intermediate affects some of the conclusions that have been drawn for GB1, a popular model for protein folding studies.
The role of the denatured state in protein folding represents a key issue for the proper evaluation of folding kinetics and mechanisms. The yeast ortholog of the human frataxin, a mitochondrial protein essential for iron homeostasis and responsible for Friedreich's ataxia, has been shown to undergo cold denaturation above 0 °C, in the absence of chemical denaturants. This interesting property provides the unique opportunity to explore experimentally the molecular mechanism of both the hot and cold denaturation. In this work, we present the characterization of the temperature and urea dependence of the folding kinetics of yeast frataxin, and show that while at neutral pH and in the absence of a denaturant a simple two-state model may satisfactorily describe the temperature dependence of the folding and unfolding rate constants, the results obtained in urea over a wide range of pH reveal an intriguing complexity, suggesting that folding of frataxin involves a broad smooth free energy barrier.
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