We used single-molecule FRET in combination with other biophysical methods and molecular simulations to investigate the effect of temperature on the dimensions of unfolded proteins. With singlemolecule FRET, this question can be addressed even under nearnative conditions, where most molecules are folded, allowing us to probe a wide range of denaturant concentrations and temperatures. We find a compaction of the unfolded state of a small cold shock protein with increasing temperature in both the presence and the absence of denaturant, with good agreement between the results from single-molecule FRET and dynamic light scattering. Although dissociation of denaturant from the polypeptide chain with increasing temperature accounts for part of the compaction, the results indicate an important role for additional temperaturedependent interactions within the unfolded chain. The observation of a collapse of a similar extent in the extremely hydrophilic, intrinsically disordered protein prothymosin ␣ suggests that the hydrophobic effect is not the sole source of the underlying interactions. Circular dichroism spectroscopy and replica exchange molecular dynamics simulations in explicit water show changes in secondary structure content with increasing temperature and suggest a contribution of intramolecular hydrogen bonding to unfolded state collapse.FRET ͉ polymer ͉ protein folding ͉ secondary structure ͉ chain dimensions T here is an increasing interest in the properties of unfolded proteins and their roles in the folding and cellular functions of proteins. A key motivation is that many proteins are marginally stable and only fold in the presence of their ligands or binding partners, opening new regulatory possibilities (1, 2). An important reason for recent progress is the growing availability of methods that provide structural information on these conformationally heterogeneous systems, such as NMR (3), scattering methods (4, 5), and single-molecule . Although NMR provides mostly local details, small-angle X-ray scattering (SAXS), dynamic light scattering (DLS), and single-molecule FRET provide overall hydrodynamic or long-range distance information. An important advantage of single-molecule FRET is the separation of folded and unfolded subpopulations (9). As a result, unfolded state properties can be investigated even in the presence of folded molecules (i.e., under near-native conditions, which are physiologically most relevant). This advance has led to the observation of a continuous collapse of the unfolded state with decreasing denaturant concentrations (10), a behavior that now has been demonstrated for a large number of proteins (11-18) and peptides (19). Recent advances in the application of theoretical models have led to a quantitative description of this unfolded state collapse in terms of polymerphysical concepts (15,(20)(21)(22)(23). Such chain compaction also has been demonstrated to result in increased internal friction and a slowdown of intramolecular dynamics of the polypeptide (19, 26), which can affect...

Förster Resonance Energy Transfer (FRET) experiments probe molecular distances via distance dependent energy transfer from an excited donor dye to an acceptor dye. Single molecule experiments not only probe average distances, but also distance distributions or even fluctuations, and thus provide a powerful tool to study biomolecular structure and dynamics. However, the measured energy transfer efficiency depends not only on the distance between the dyes, but also on their mutual orientation, which is typically inaccessible to experiments. Thus, assumptions on the orientation distributions and averages are usually made, limiting the accuracy of the distance distributions extracted from FRET experiments. Here, we demonstrate that by combining single molecule FRET experiments with the mutual dye orientation statistics obtained from Molecular Dynamics (MD) simulations, improved estimates of distances and distributions are obtained. From the simulated time-dependent mutual orientations, FRET efficiencies are calculated and the full statistics of individual photon absorption, energy transfer, and photon emission events is obtained from subsequent Monte Carlo (MC) simulations of the FRET kinetics. All recorded emission events are collected to bursts from which efficiency distributions are calculated in close resemblance to the actual FRET experiment, taking shot noise fully into account. Using polyproline chains with attached Alexa 488 and Alexa 594 dyes as a test system, we demonstrate the feasibility of this approach by direct comparison to experimental data. We identified cis-isomers and different static local environments as sources of the experimentally observed heterogeneity. Reconstructions of distance distributions from experimental data at different levels of theory demonstrate how the respective underlying assumptions and approximations affect the obtained accuracy. Our results show that dye fluctuations obtained from MD simulations, combined with MC single photon kinetics, provide a versatile tool to improve the accuracy of distance distributions that can be extracted from measured single molecule FRET efficiencies.

Molecular chaperones are known to be essential for avoiding protein aggregation in vivo, but it is still unclear how they affect protein folding mechanisms. We use single-molecule Förster resonance energy transfer to follow the folding of a protein inside the GroEL/GroES chaperonin cavity over a time range from milliseconds to hours. Our results show that confinement in the chaperonin decelerates the folding of the C-terminal domain in the substrate protein rhodanese, but leaves the folding rate of the N-terminal domain unaffected. Microfluidic mixing experiments indicate that strong interactions of the substrate with the cavity walls impede the folding process, but the folding hierarchy is preserved. Our results imply that no universal chaperonin mechanism exists. Rather, a competition between intra-and intermolecular interactions determines the folding rates and mechanisms of a substrate inside the GroEL/GroES cage.I n the recent past, a large number of components have been identified that control and modulate protein folding in vivo. This machinery includes molecular chaperones (1-3), sophisticated quality control systems, and complex mechanisms for protein translocation and degradation (3, 4), reflecting the importance of regulating the delicate balance of protein folding, misfolding, and aggregation in the cell. Such cellular factors exert conformational constraints on protein molecules that are expected to have a strong effect on the corresponding free-energy surfaces for folding (5). However, while the combination of cellular, biochemical, and structural data has led to some plausible qualitative models for the processes involved, mechanistic investigations comparable to those of autonomous protein folding in vitro (5-8) have been complicated by the complexity of the systems and the conformational heterogeneity involved (9). Even the autonomous folding of chaperone substrate proteins has been difficult to investigate because of their strong aggregation tendency (10). Contributions from confinement and crowding have been addressed in numerous studies using molecular simulations and theory (11)(12)(13)(14)(15)(16)(17)(18)(19)(20), but many of these concepts have eluded experimental examination.Here, we take a step towards closing this gap by investigating the GroEL/GroES chaperonin (1-3, 9) with single-molecule fluorescence spectroscopy (21-24), a method that is starting to provide previously inaccessible information on chaperonemediated protein folding (25)(26)(27)(28)(29)(30). GroEL/GroES is a remarkable molecular machine that binds nonnative proteins and allows them to fold within a cavity formed by the heptameric rings of GroEL and GroES. However, the cavity is only slightly larger than the folded structure of typical proteins known to interact with the chaperonin. The large volume of unconfined unfolded protein chains compared to the size of the cavity raises the question of whether and how such strong confinement affects the folding reaction (12-16, 18, 31, 32). By labeling the classic substrate prote...

Single-molecule Förster resonance energy transfer (FRET) and photoinduced electron transfer (PET) have developed into versatile and complementary methods for probing distances and dynamics in biomolecules. Here we show that the two methods can be combined in one molecule to obtain both accurate distance information and the kinetics of intramolecular contact formation. In a first step, we show that the fluorescent dyes Alexa 488 and Alexa 594, which are frequently used as a donor and acceptor for single-molecule FRET, are also suitable as PET probes with tryptophan as a fluorescence quencher. We then performed combined FRET/PET experiments with FRET donor- and acceptor-labeled polyproline peptides. The placement of a tryptophan residue into the polyglycylserine tail incorporated in the peptides allowed us to measure both FRET efficiencies and the nanosecond dynamics of contact formation between one of the fluorescent dyes and the quencher. Variation of the linker length between the polyproline and the Alexa dyes and in the position of the tryptophan residue demonstrates the sensitivity of this approach. Modeling of the combined photon statistics underlying the combined FRET and PET process enables the accurate analysis of both the resulting transfer efficiency histograms and the nanosecond fluorescence correlation functions. This approach opens up new possibilities for investigating single biomolecules with high spatial and temporal resolution.

Background The kidney proximal convoluted tubule (PCT) reabsorbs filtered macromolecules via receptor-mediated endocytosis (RME) or nonspecific fluid phase endocytosis (FPE); endocytosis is also an entry route for disease-causing toxins. PCT cells express the protein ligand receptor megalin and have a highly developed endolysosomal system (ELS). Two PCT segments (S1 and S2) display subtle differences in cellular ultrastructure; whether these translate into differences in endocytotic function has been unknown.Methods To investigate potential differences in endocytic function in S1 and S2, we quantified ELS protein expression in mouse kidney PCTs using real-time quantitative polymerase chain reaction and immunostaining. We also used multiphoton microscopy to visualize uptake of fluorescently labeled ligands in both living animals and tissue cleared using a modified CLARITY approach.Results Uptake of proteins by RME occurs almost exclusively in S1. In contrast, dextran uptake by FPE takes place in both S1 and S2, suggesting that RME and FPE are discrete processes. Expression of key ELS proteins, but not megalin, showed a bimodal distribution; levels were far higher in S1, where intracellular distribution was also more polarized. Tissue clearing permitted imaging of ligand uptake at singleorganelle resolution in large sections of kidney cortex. Analysis of segmented tubules confirmed that, compared with protein uptake, dextran uptake occurred over a much greater length of the PCT, although individual PCTs show marked heterogeneity in solute uptake length and three-dimensional morphology.Conclusions Striking axial differences in ligand uptake and ELS function exist along the PCT, independent of megalin expression. These differences have important implications for understanding topographic patterns of kidney diseases and the origins of proteinuria.