Subdomain-Specific Collapse of Denatured Staphylococcal Nuclease Revealed by Single Molecule Fluorescence Resonance Energy Transfer Measurements

Conformational Dynamics of the Periplasmic Chaperone SurA

The periplasmic protein SurA is the primary chaperone involved in the biogenesis of bacterial outer membrane proteins and is a potential antibacterial drug target. The three-dimensional structure of SurA can be divided into three parts, a core module formed by the N- and C-terminal regions and two peptidyl-prolyl isomerase (PPIase) domains, P1 and P2. Despite the determination of the structures of several SurA-peptide complexes, the functional mechanism of this chaperone remains elusive and the roles of the two PPIase domains are yet unclear. Herein, we characterize the conformational dynamics of SurA by using solution nuclear magnetic resonance and single-molecule fluorescence resonance energy transfer methods. We demonstrate a "closed-to-open" structural transition of the P1 domain that is correlated with both chaperone activity and peptide binding and show that the flexible P2 domain can also occupy conformations that closely contact the NC core module. Our results offer a structural basis for the counteracting roles of the two PPIase domains in regulating the SurA chaperone activity.

Single-Molecule Detection Reveals Different Roles of Skp and SurA as Chaperones

Skp and SurA are both periplasmic chaperones involved in the biogenesis of Escherichia coli β-barrel outer membrane proteins (OMPs). It is commonly assumed that SurA plays a major role whereas Skp is a minor factor. However, there is no molecular evidence for whether their roles are redundant. Here, by using different dilution methods, we obtained monodisperse and aggregated forms of OmpC and studied their interactions with Skp and SurA by single-molecule fluorescence resonance energy transfer and fluorescence correlation spectroscopy. We found that Skp can dissolve aggregated OmpC while SurA cannot convert aggregated OmpC into the monodisperse form and the conformations of OmpC recognized by the two chaperones as well as their stoichiometries of binding are different. Our study demonstrates the functional distinctions between Skp and SurA. In particular, the role of Skp is not redundant and is probably more significant under stress conditions.

Shedding light on protein folding landscapes by single-molecule fluorescence

Single-molecule (SM) fluorescence methods have been increasingly instrumental in our current understanding of a number of key aspects of protein folding and aggregation landscapes over the past decade. With the advantage of a model free approach and the power of probing multiple subpopulations and stochastic dynamics directly in a heterogeneous structural ensemble, SM methods have emerged as a principle technique for studying complex systems such as intrinsically disordered proteins (IDPs), globular proteins in the unfolded basin and during folding, and early steps of protein aggregation in amyloidogenesis. This review highlights the application of these methods in investigating the free energy landscapes, folding properties and dynamics of individual protein molecules and their complexes, with an emphasis on inherently flexible systems such as IDPs.

The pH dependence of staphylococcal nuclease stability is incompatible with a three-state denaturation model

Six single substitution mutations, V66F, V66G, V66N, V66Q, V66S, V66T, and V66Y, were made in the background of a highly stable triple mutant (P117G, H124L, and S128A) of staphylococcal nuclease. The thermodynamic stabilities of wild type staphylococcal nuclease, of the stable triple mutant and of its six variants were determined by guanidine hydrochloride denaturation in thirteen different buffers spanning the pH range 4.5 to 10.2. Within experimental error the values of [Formula: see text] and mGuHCl for the various proteins measured over this wide range of pH maintain a constant offset from one another, tracing a series of approximately parallel curves. This data offers an independent means of determining the error of stabilities and slopes determined by guanidine hydrochloride denaturations and shows that previous error estimates are accurate. More importantly, this behavior cannot be reconciled with a three-state denaturation model for staphylococcal nuclease. The large variations in mGuHCl observed in these mutants must therefore arise from other causes.

Single-molecule detection reveals knot sliding in TrmD denaturation

An increasing number of proteins are found to contain a knot in their polypeptide chain. Although some studies have looked into the folding mechanism of knotted proteins, why and how these complex topologies form are still far from being fully answered. Moreover, no experimental information about how the knot moves during the protein-folding process is available. Herein, by combining single-molecule fluorescence resonance energy transfer (smFRET) experiments with molecular dynamics (MD) simulations, we performed a detailed study to characterize the knot in the denatured state of TrmD, a knotted tRNA (guanosine-1) methyltransferase from Escherichia coli, as a model system. We found that the knot still existed in the unfolded state of TrmD, consistent with the results for two other knotted proteins, YibK and YbeA. More interestingly, both smFRET experiments and MD simulations revealed that the knot slid towards the C-terminal during the unfolding process, which could be explained by the relatively strong interactions between the β-sheet core at the N terminal of the native knot region. The size of the knot in the unfolded state is not larger than that in the native state. In addition, the knot slid in a "downhill" mode with simultaneous chain collapse in the denatured state.

How, when and why proteins collapse: the relation to folding

Unfolded proteins under strongly denaturing conditions are highly expanded. However, when the conditions are more close to native, an unfolded protein may collapse to a compact globular structure distinct from the folded state. This transition is akin to the coil-globule transition of homopolymers. Single-molecule FRET experiments have been particularly conducive in revealing the collapsed state under conditions of coexistence with the folded state. The collapse can be even more readily observed in natively unfolded proteins. Time-resolved studies, using FRET and small-angle scattering, have shown that the collapse transition is a very fast event, probably occurring on the submicrosecond time scale. The forces driving collapse are likely to involve both hydrophobic and backbone interactions. The loss of configurational entropy during collapse makes the unfolded state less stable compared to the folded state, thus facilitating folding.

Protein folding at single-molecule resolution

The protein folding reaction carries great significance for cellular function and hence continues to be the research focus of a large interdisciplinary protein science community. Single-molecule methods are providing new and powerful tools for dissecting the mechanisms of this complex process by virtue of their ability to provide views of protein structure and dynamics without associated ensemble averaging. This review briefly introduces common FRET and force methods, and then explores several areas of protein folding where single-molecule experiments have yielded insights. These include exciting new information about folding landscapes, dynamics, intermediates, unfolded ensembles, intrinsically disordered proteins, assisted folding and biomechanical unfolding. Emerging and future work is expected to include advances in single-molecule techniques aimed at such investigations, and increasing work on more complex systems from both the physics and biology standpoints, including folding and dynamics of systems of interacting proteins and of proteins in cells and organisms. This article is part of a Special Issue entitled: Protein Dynamics: Experimental and Computational Approaches.

Direct measurement of the rates and barriers on forward and reverse diffusions of intramolecular collision in overhang oligonucleotides

The dynamics of end-to-interior (Type I) and end-to-end (Type II) collisions in a dangling overhang anchored on a double-stranded DNA (dsDNA) was studied by monitoring the fluorescence quenching of tetramethylrhodamine (TMR) by guanosine residues through combining photoinduced electron transfer (PET) with fluorescence correlation spectroscopy (FCS) at different temperatures. TMR and guanosine residues are separated by a double helix with dangling bases ranging from 2 to 16. By analyzing the FCS data, we obtained the forward and reverse intrachain diffusion rate constants and respective barriers. For both Type I and Type II collisions, the intrachain diffusion rates followed the scaling law of the Gaussian chain model. Especially, the reverse intrachain diffusion rate was insensitive to the base length of separation. Both the activation enthalpy and activation entropy of the forward and reverse diffusions were length independent. The comparison between Type I and Type II collisions shows that the collision rate of end-to-interior is slower than that of end-to-end. The phenomenon is further checked in detail by a series of dangling DNA with the same separation length but different tail lengths (Type III).

Single-molecule studies of the Im7 folding landscape

Under appropriate conditions, the four-helical Im7 (immunity protein 7) folds from an ensemble of unfolded conformers to a highly compact native state via an on-pathway intermediate. Here, we investigate the unfolded, intermediate, and native states populated during folding using diffusion single-pair fluorescence resonance energy transfer by measuring the efficiency of energy transfer (or proximity or P ratio) between pairs of fluorophores introduced into the side chains of cysteine residues placed in the center of helices 1 and 4, 1 and 3, or 2 and 4. We show that while the native states of each variant give rise to a single narrow distribution with high P values, the distributions of the intermediates trapped at equilibrium (denoted I^eqm) are fitted by two Gaussian distributions. Modulation of the folding conditions from those that stabilize the intermediate to those that destabilize the intermediate enabled the distribution of lower P value to be assigned to the population of the unfolded ensemble in equilibrium with the intermediate state. The reduced stability of the I^eqm variants allowed analysis of the effect of denaturant concentration on the compaction and breadth of the unfolded state ensemble to be quantified from 0 to 6 M urea. Significant compaction is observed as the concentration of urea is decreased in both the presence and absence of sodium sulfate, as previously reported for a variety of proteins. In the presence of Na₂SO₄ in 0 M urea, the P value of the unfolded state ensemble approaches that of the native state. Concurrent with compaction, the ensemble displays increased peak width of P values, possibly reflecting a reduction in the rate of conformational exchange among iso-energetic unfolded, but compact conformations. The results provide new insights into the initial stages of folding of Im7 and suggest that the unfolded state is highly conformationally constrained at the outset of folding.