Small-Angle X-ray Scattering and Single-Molecule FRET Spectroscopy Produce Highly Divergent Views of the Low-Denaturant Unfolded State

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Small-angle scattering studies generally indicate that the dimensions of unfolded single-domain proteins are independent (to within experimental uncertainty of a few percent) of denaturant concentration. In contrast, single-molecule FRET (smFRET) studies invariably suggest that protein unfolded states contract significantly as the denaturant concentration falls from high (∼6 M) to low (∼1 M). Here, we explore this discrepancy by using PEG to perform a hitherto absent negative control. This uncharged, highly hydrophilic polymer has been shown by multiple independent techniques to behave as a random coil in water, suggesting that it is unlikely to expand further on the addition of denaturant. Consistent with this observation, small-angle neutron scattering indicates that the dimensions of PEG are not significantly altered by the presence of either guanidine hydrochloride or urea. smFRET measurements on a PEG construct modified with the most commonly used FRET dye pair, however, produce denaturant-dependent changes in transfer efficiency similar to those seen for a number of unfolded proteins. Given the vastly different chemistries of PEG and unfolded proteins and the significant evidence that dye-free PEG is well-described as a denaturant-independent random coil, this similarity raises questions regarding the interpretation of smFRET data in terms of the hydrogen bond-or hydrophobically driven contraction of the unfolded state at low denaturant.protein folding | SAXS | two state | statistical coil | Flory scaling R ecent years have seen a significant controversy arise regarding the behavior of the unfolded states of single-domain proteins in response to changing levels of chemical denaturant. That is, although small-angle X-ray scattering (SAXS) and single-molecule FRET (smFRET) results are all consistent with the argument that, at high levels of chemical denaturant (∼6 M or above), unfolded proteins adopt a swollen, self-avoiding ensemble well-approximated as an excluded volume random coil (1-3), the two approaches produce seemingly discrepant results for the dimensions of the unfolded states populated at lower (∼1 M) denaturant (4). For example, time-resolved SAXS studies of the unfolded state transiently populated when protein L is rapidly shifted from high guanidine hydrochloride (GuHCl) to low denaturant conditions produce no experimentally significant evidence for the compaction of this single-domain protein before folding (4, 5) [e.g., estimated radii of gyration of 25.1 ± 0.3 Å for the unfolded state at equilibrium in 7 M GuHCl and 24.9 ± 1.1 Å for the transient unfolded state populated at 0.67 M GuHCl; confidence intervals are SEs (4)]. In contrast, multiple smFRET studies conducted at equilibrium suggest that the unfolded state of dye-labeled protein L contracts by 20-40% over this same range of denaturant concentrations (6, 7) (Fig.

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confidence: 72%

“…Again, the source of this experimentally robust discrepancy remains stubbornly unclear (a more detailed discussion of this issue is in ref. 4).…”

Section: Significancementioning

confidence: 99%

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confidence: 99%

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Random coil negative control reproduces the discrepancy between scattering and FRET measurements of denatured protein dimensions

Watkins

Simon

Sosnick

et al. 2015

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“…This equivalence indicates that the two methods probe the same folding transition to a DSE that is devoid of stable H bonds. Moreover, data from small-angle X-ray scattering imply that the dimensions in the DSE of many [but not all (56,57)] small proteins remain unchanged upon shifting to a lower level of denaturant (32,(58)(59)(60). Furthermore, most [but not all (61)] small proteins satisfy the two-state chevron criterion, sometimes even down to 0 M denaturant (21,22), indicating that the DSE remains highly solvated under native conditions for many proteins.…”

Section: Discussionmentioning

confidence: 99%

Cooperative folding near the downhill limit determined with amino acid resolution by hydrogen exchange

Baxa

Gagnon

et al. 2016

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The relationship between folding cooperativity and downhill, or barrier-free, folding of proteins under highly stabilizing conditions remains an unresolved topic, especially for proteins such as λ-repressor that fold on the microsecond timescale. Under aqueous conditions where downhill folding is most likely to occur, we measure the stability of multiple H bonds, using hydrogen exchange (HX) in a λ YA variant that is suggested to be an incipient downhill folder having an extrapolated folding rate constant of 2 × 10 5 s −1 and a stability of 7.4 kcal·mol −1 at 298 K. At least one H bond on each of the three largest helices (α1, α3, and α4) breaks during a common unfolding event that reflects global denaturation. The use of HX enables us to both examine folding under highly stabilizing, native-like conditions and probe the pretransition state region for stable species without the need to initiate the folding reaction. The equivalence of the stability determined at zero and high denaturant indicates that any residual denatured state structure minimally affects the stability even under native conditions. Using our ψ analysis method along with mutational ϕ analysis, we find that the three aforementioned helices are all present in the folding transition state. Hence, the free energy surface has a sufficiently high barrier separating the denatured and native states that folding appears cooperative even under extremely stable and fast folding conditions. T he nature of the energy landscape when folding occurs on the microsecond timescale continues to be investigated using both experimental and computational approaches. The 80-residue subdomain of the λ-repressor transcription factor, λ 6-85 (1-11), is an appealing system as it contains five α-helices arranged in a nonsymmetric pattern, folds in microseconds, and is nearly a downhill folder (12), a condition where a continuous series of folding events may be characterized. These characteristics along with a folding time that nears the upper limit for current all-atom simulations (13-19) make this protein appropriate for detailed comparisons between experiment and simulations.The energy landscape of λ 6-85 is significantly influenced by its sequence. Oas and coworkers found that the wild type and a fasterfolding mutant with two helix-promoting substitutions (λ AA with G46A/G48A, Fig. S1A) fold cooperatively (1-4). The transition state ensemble (TSE) characterized using ϕ analysis minimally contains α1 and α4 (3). Kinetic H/D isotope effect measurements in the Sosnick laboratory found that both λ 6-85 and λ AA fold cooperatively with ∼70% of the H bonds being formed in the TSE, matching the degree of surface buried in the TSE [beta Tanford value (β Tanford )] (5).Using nanosecond T-jump and other methods, Gruebele and coworkers proposed that faster-folding and stabilized variants, such as λ YA (λ AA + Q33Y) and λ D14A (λ YA + D14A), fold in an incipient or fully downhill manner, especially under highly stable conditions at lower temperatures (6-9). Key signatures of downhi...

“…Despite their obvious complementarity, SAXS, NMR, and single-molecule FRET data on unfolded proteins or IDPs have only rarely been directly combined or compared, and concerns have been raised about the validity of the individual methods for correctly quantifying unfolded-state properties (36,37). Here we present a direct comparison of the properties of urea-denatured ubiquitin as quantified from all three methods and enhance the description of the ensemble by the FRET-specific single-molecule, time-dependent, and long-range distance information.…”

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confidence: 99%

Comprehensive structural and dynamical view of an unfolded protein from the combination of single-molecule FRET, NMR, and SAXS

Aznauryan

Delgado

Soranno

et al. 2016

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The properties of unfolded proteins are essential both for the mechanisms of protein folding and for the function of the large group of intrinsically disordered proteins. However, the detailed structural and dynamical characterization of these highly dynamic and conformationally heterogeneous ensembles has remained challenging. Here we combine and compare three of the leading techniques for the investigation of unfolded proteins, NMR spectroscopy (NMR), smallangle X-ray scattering (SAXS), and single-molecule Förster resonance energy transfer (FRET), with the goal of quantitatively testing their consistency and complementarity and for obtaining a comprehensive view of the unfolded-state ensemble. Using unfolded ubiquitin as a test case, we find that its average dimensions derived from FRET and from structural ensembles calculated using the program X-PLOR-NIH based on NMR and SAXS restraints agree remarkably well; even the shapes of the underlying intramolecular distance distributions are in good agreement, attesting to the reliability of the approaches. The NMR-based results provide a highly sensitive way of quantifying residual structure in the unfolded state. FRETbased nanosecond fluorescence correlation spectroscopy allows long-range distances and chain dynamics to be probed in a time range inaccessible by NMR. The combined techniques thus provide a way of optimally using the complementarity of the available methods for a quantitative structural and dynamical description of unfolded proteins both at the global and the local level.protein folding | unfolded protein ensemble | Förster resonance energy transfer | nuclear magnetic resonance | small-angle X-ray scattering P roteins exist as ensembles of interconverting conformations.Obviously, unfolded polypeptide chains, such as chemically or physically denatured proteins and intrinsically disordered proteins (IDPs), can access extremely large numbers of conformations (1). A comprehensive description of their structural and dynamical behavior is a prerequisite for understanding protein folding (2-4) and the function of IDPs in health and disease (5, 6). Due to the very large number of conformational degrees of freedom of the unfolded polypeptide ensemble, it is of utmost importance to obtain as many independent experimental parameters as possible for a quantitative description of its behavior. Three experimental methods have been particularly informative in this respect: NMR spectroscopy (2, 5, 7-9), small angle X-ray scattering (SAXS) (10, 11), and single-molecule Förster resonance energy transfer spectroscopy (single-molecule FRET) (12, 13).NMR in solution provides very rich local structural and dynamical information at virtually any atom site with the exception of oxygen. Distance and angular information can be obtained from nuclear Overhauser enhancements (14), three-bond scalar couplings (15), paramagnetic relaxation enhancements (PREs) (16), pseudo contact shifts (17), residual dipolar couplings (RDCs) (8, 18), chemical shifts (19), and hydrogen bond scalar ...