NOE data demonstrating a compact unfolded state for an SH3 domain under non-denaturing conditions

Early events in protein folding: Is there something more than hydrophobic burst?

The presence of native contacts in the denatured state of many proteins suggests that elements of the biologically active structure of these molecules are formed during the initial stage of the folding process. The rapidity with which these events take place makes it difficult to study them in vitro, but, by the same token, suitable for studies in silico. With the help of all-atom, explicit solvent, molecular dynamics simulations we have followed in time, starting from elongated structureless conformations, the early events in the folding of src-SH3 domain and of proteins G, L, and CI2. It is observed that within the first 50 ns two important events take place, essentially independent of each other: hydrophobic collapse and formation of a few selected native contacts. The same contacts are also found in simulations carried out in the presence of guanidinium chloride in order to reproduce the conditions used to characterize experimentally the denatured state and testify to the fact that these contacts are to be considered a resilient characterizing property of the denaturated state.

Denatured state is critical in determining the properties of model proteins designed on different folds

The thermodynamics of proteins designed on three common folds (SH3, chymotrypsin inhibitor 2 [CI2], and protein G) is studied with a simplified C(alpha) model and compared with the thermodynamics of proteins designed on random-generated folds. The model allows to design sequences to fold within a dRMSD ranging from 1.2 to 4.2 A from the crystallographic native conformation and to study properties that are hard to be measured experimentally. It is found that the denatured state of all of them is not random but is, to different extents, partially structured. The degree of structure is more abundant for SH3 and protein G, giving rise to a weaker stability but a more efficient folding kinetics than CI2 and, even more, than the random-generated folds. Consequently, the features of the unfolded state seem to be as important in the determination of the thermodynamic properties of these proteins as the features of the native state.

Electrostatic interactions in the denatured state ensemble: their effect upon protein folding and protein stability

It is now recognized that the denatured state ensemble (DSE) of proteins can contain significant amounts of structure, particularly under native conditions. Well-studied examples include small units of hydrogen bonded secondary structure, particularly helices or turns as well as hydrophobic clusters. Other types of interactions are less well characterized and it has often been assumed that electrostatic interactions play at most a minor role in the DSE. However, recent studies have shown that both favorable and unfavorable electrostatic interactions can be formed in the DSE. These can include surprisingly specific non-native interactions that can even persist in the transition state for protein folding. DSE electrostatic interactions can be energetically significant and their modulation either by mutation or by varying solution conditions can have a major impact upon protein stability. pH dependent stability studies have shown that electrostatic interactions can contribute up to 4 kcal mol(-1) to the stability of the DSE.

Tryptophan fluorescence reveals the presence of long-range interactions in the denatured state of ribonuclease Sa

Characterizing the denatured state ensemble is crucial to understanding protein stability and the mechanism of protein folding. The aim of this research was to see if fluorescence could be used to gain new information on the denatured state ensemble. Ribonuclease Sa (RNase Sa) contains no Trp residues. We made five variants of RNase Sa by adding Trp residues at locations where they are found in other members of the microbial ribonuclease family. To better understand the protein denatured state, we also studied the fluorescence properties of the following peptides: N-acetyl-Trp-amide (NATA), N-acetyl-Ala-Trp-Ala-amide (AWA), N-acetyl-Ala-Ala-Trp-Ala-Ala-amide (AAWAA), and the five pentapeptides with the same sequence as the Trp substitution sites in RNase Sa. The major conclusions are: 1), the wavelength of maximum fluorescence intensity, lambda(max), does not differ significantly for the peptides and the denatured proteins; 2), the fluorescence intensity at lambda(max), I(F), differs significantly for the five Trp containing variants of RNase Sa; 3), the I(F) differences for the denatured proteins are mirrored in the peptides, showing that the short-range effects giving rise to the I(F) differences in the peptides are also present in the proteins; 4) the I(F) values for the denatured proteins are more than 30% greater than for the peptides, showing the presence of long-range effects in the proteins; 5), fluorescence quenching of Trp by acrylamide and iodide is more than 50% greater in the peptides than in the denatured proteins, showing that long-range effects limit the accessibility of the quenchers to the Trp side chains in the proteins; and 6), these results show that nonlocal effects in the denatured states of proteins influence Trp fluorescence and accessibility significantly.

Theoretical framework for NMR residual dipolar couplings in unfolded proteins

A theoretical framework for the prediction of nuclear magnetic resonance (NMR) residual dipolar couplings (RDCs) in unfolded proteins under weakly aligning conditions is presented. The unfolded polypeptide chain is modeled as a random flight chain while the alignment medium is represented by a set of regularly arranged obstacles. For the case of bicelles oriented perpendicular to the magnetic field, a closed-form analytical result is derived. With the obtained analytical expression the RDCs are readily accessible for any locus along the chain, for chains of differing length, and for varying bicelle concentrations. The two general features predicted by the model are (i) RDCs in the center segments of a polypeptide chain are larger than RDCs in the end segments, resulting in a bell-shaped sequential distribution of RDCs, and (ii) couplings are larger for shorter chains than for longer chains at a given bicelle concentration. Experimental data available from the literature confirm the first prediction of the model, providing a tool for recognizing fully unfolded polypeptide chains. With less certainty experimental data appear to support the second prediction as well. However, more systematic experimental studies are needed in order to validate or disprove the predictions of the model. The presented framework is an important step towards a solid theoretical foundation for the analysis of experimentally measured RDCs in unfolded proteins in the case of alignment media such as polyacrylamide gels and neutral bicelle systems which align biomacromolecules by a steric mechanism. Various improvements and generalizations are possible within the suggested approach.

Improved Structural Characterizations of the drkN SH3 Domain Unfolded State Suggest a Compact Ensemble with Native-like and Non-native Structure

Due to their dynamic ensemble nature and a deficiency of experimental restraints, disordered states of proteins are difficult to characterize structurally. Here, we have expanded upon our previous work on the unfolded state of the Drosophila drk N-terminal (drkN) SH3 domain with our program ENSEMBLE, which assigns population weights to pregenerated conformers in order to calculate ensembles of structures whose properties are collectively consistent with experimental measurements. The experimental restraint set has been enlarged with newly measured paramagnetic relaxation enhancements from Cu(2+) bound to an amino terminal Cu(2+)-Ni(2+) binding (ATCUN) motif as well as nuclear Overhauser effect (NOE) and hydrogen exchange data from recent studies. In addition, two new pseudo-energy minimization algorithms have been implemented that have dramatically improved the speed of ENSEMBLE population weight assignment. Finally, we have greatly improved our conformational sampling by utilizing a variety of techniques to generate both random structures and structures that are biased to contain elements of native-like or non-native structure. Although it is not possible to uniquely define a representative structural ensemble, we have been able to assess various properties of the drkN SH3 domain unfolded state by performing ENSEMBLE minimizations of different conformer pools. Specifically, we have found that the experimental restraint set enforces a compact structural distribution that is not consistent with an overall native-like topology but shows preference for local non-native structure in the regions corresponding to the diverging turn and the beta5 strand of the folded state and for local native-like structure in the region corresponding to the beta6 and beta7 strands. We suggest that this approach could be generally useful for the structural characterization of disordered states.

The Cold Denatured State Is Compact but Expands at Low Temperatures: Hydrodynamic Properties of the Cold Denatured State of the C-terminal Domain of L9

A point mutation of a small globular protein, the C-terminal domain of L9 destabilizes the protein and leads to observable cold-denaturation at temperatures above zero. The cold denatured state is in slow exchange with the native state on the NMR time scale, and this allows the hydrodynamic properties of the cold unfolded state and the native state to be measured under identical conditions using pulsed-field gradient NMR diffusion measurements. This provides the first experimental measurement of the hydrodynamic properties of a cold unfolded protein and its folded form under identical conditions. Hydrodynamic radii of the cold-induced unfolded states were measured for a set of temperatures ranging from 2 degrees C to 25 degrees C at pD 6.6 in the absence of denaturant. The cold unfolded state is compact compared to the urea or acid unfolded state and a trend of increasing radii of hydration is observed as the temperature is lowered. These observations are confirmed by experiments on the same protein at pD 8.0, where it is more stable, in the presence of a modest concentration of urea. The expansion of the cold-denatured state at lower temperatures is consistent with the temperature dependence of hydrophobic interactions.

Thermodynamics of protein denatured states

Recent work on the thermodynamics of protein denatured states is providing insight into the stability of residual structure and the conformational constraints that affect the disordered states of proteins. Current data from native state hydrogen exchange and the pH dependence of protein stability indicate that residual structure can modulate the stability of the denatured state by up to 4 kcal mol(-1). NMR structural data have emphasized the role of hydrophobic clusters in stabilizing denatured state residual structures, however recent results indicate that electrostatic interactions, both favorable and unfavorable, are also important modulators of the stability of the denatured state. Thermodynamics methods that take advantage of histidine-heme ligation chemistry have also been developed to probe the conformational constraints that act on denatured states. These methods have provided insights into the role of excluded volume, chain stiffness, and loop persistence in modulating the conformational preferences of highly disordered proteins. New insights into protein folding and novel methods to manipulate protein stability are emerging from this work.

Interplay of secondary structures and side-chain contacts in the denatured state of BBA1

The denatured state of a miniprotein BBA1 is studied under the native condition with the AMBER/Poisson-Boltzmann energy model and with the self-guided enhanced sampling technique. Forty independent trajectories are collected to sample the highly diversified denatured structures. Our simulation data show that the denatured BBA1 contains high percentage of native helix and native turn, but low percentage of native hairpin. Conditional population analysis indicates that the native helix formation and the native hairpin formation are not cooperative in the denatured state. Side-chain analysis shows that the native hydrophobic contacts are more preferred than the non-native hydrophobic contacts in the denatured BBA1. In contrast, the salt-bridge contacts are more or less nonspecific even if their populations are higher than those of hydrophobic contacts. Analysis of the trajectories shows that the native helix mostly initiates near the N terminus and propagates to the C terminus, and mostly forms from 3(10)-helix/turn to alpha helix. The same analysis shows that the native turn is important but not necessary in its formation in the denatured BBA1. In addition, the formations of the two strands in the native hairpin are rather asymmetric, demonstrating the likely influence of the protein environment. Energetic analysis shows that the native helix formation is largely driven by electrostatic interactions in denatured BBA1. Further, the native helix formation is associated with the breakup of non-native salt-bridge contacts and the accumulation of native salt-bridge contacts. However, the native hydrophobic contacts only show a small increase upon the native helix formation while the non-native hydrophobic contacts stay essentially the same, different from the evolution of hydrophobic contacts observed in an isolated helix folding.

GroEL-mediated protein folding: making the impossible, possible

Protein folding is a spontaneous process that is essential for life, yet the concentrated and complex interior of a cell is an inherently hostile environment for the efficient folding of many proteins. Some proteins-constrained by sequence, topology, size, and function-simply cannot fold by themselves and are instead prone to misfolding and aggregation. This problem is so deeply entrenched that a specialized family of proteins, known as molecular chaperones, evolved to assist in protein folding. Here we examine one essential class of molecular chaperones, the large, oligomeric, and energy utilizing chaperonins or Hsp60s. The bacterial chaperonin GroEL, along with its co-chaperonin GroES, is probably the best-studied example of this family of protein-folding machine. In this review, we examine some of the general properties of proteins that do not fold well in the absence of GroEL and then consider how folding of these proteins is enhanced by GroEL and GroES. Recent experimental and theoretical studies suggest that chaperonins like GroEL and GroES employ a combination of protein isolation, unfolding, and conformational restriction to drive protein folding under conditions where it is otherwise not possible.

Motional properties of unfolded ubiquitin: a model for a random coil protein

The characterization of unfolded states of proteins has recently attracted considerable interest, as the residual structure present in these states may play a crucial role in determining their folding and misfolding behavior. Here, we investigated the dynamics in the denatured state of ubiquitin in 8 M urea at pH2. Under these conditions, ubiquitin does not have any detectable local residual structure, and uniform 15N relaxation rates along the sequence indicate the absence of motional restrictions caused by residual secondary structure and/or long-range interactions. A comparison of different models to predict relaxation data in unfolded proteins suggests that the subnanosecond dynamics in unfolded states depend on segmental motions only and do not show a dependence on the residue type but for proline and glycine residues.

Thermodynamic features characterizing good and bad folding sequences obtained using a simplified off-lattice protein model

The thermodynamics of the small SH3 protein domain is studied by means of a simplified model where each beadlike amino acid interacts with the others through a contact potential controlled by a random matrix. Good folding sequences, characterized by a low native energy, display three main thermodynamical ensembles, namely, a coil-like ensemble, an unfolded globule, and a folded ensemble (plus two other states, frozen and random coils, populated only at extreme temperatures). Interestingly, the unfolded globule has some regions already structured. Poorly designed sequences, on the other hand, display a wide transition from the random coil to a frozen state. The comparison with the analytic theory of heteropolymers is discussed.

Partial unfolding of diverse SH3 domains on a wide timescale

SH3 domains are small, modular domains that are found in many proteins, especially signal transduction proteins such as tyrosine kinases. While much is known about the sequences and tertiary structures of SH3 domains, far less is known about their solution dynamics. A slow, partial unfolding event that occurs under physiological conditions was previously identified in the Hck SH3 domain using hydrogen exchange (HX) mass spectrometry (MS). To determine if this unfolding was unique to Hck SH3, HX MS was used to analyze 11 other SH3 domains: seven SH3 domains from Src-family kinases and five SH3 domains from various proteins. A wide variety of unfolding rates were found, with unfolding half-lives ranging from 1s to 1h. The Lyn and alpha-spectrin SH3 domains exhibited slow, partial unfolding in beta strands D and E and part of the RT-loop. Hck SH3 also underwent partial unfolding in the same region, implying that a unique feature in this area of the domains is responsible for the partial unfolding. Partial unfolding was, however, not a function of sequence conservation. Although the Fyn and Yes SH3 domains are very similar to Hck SH3 in sequence, they exhibited no evidence of partial unfolding. Overall, the results suggest that while the tertiary structure of SH3 domains is highly conserved, the dynamics of SH3 domains are variable.

Characterizing a Partially Folded Intermediate of the Villin Headpiece Domain Under Non-denaturing Conditions: Contribution of His41 to the pH-dependent Stability of the N-terminal Subdomain

The contribution of interactions involving the imidazole ring of His41 to the pH-dependent stability of the villin headpiece (HP67) N-terminal subdomain has been investigated by nuclear magnetic resonance (NMR) spin relaxation. NMR-derived backbone N-H order parameters (S2) for wild-type (WT) HP67 and H41Y HP67 indicate that reduced conformational flexibility of the N-terminal subdomain in WT HP67 is due to intramolecular interactions with the His41 imidazole ring. These interactions, together with desolvation effects, contribute to significantly depress the pKa of the buried imidazole ring in the native state. 15N R1rho relaxation dispersion data indicate that WT HP67 populates a partially folded intermediate state that is 10.9 kJ mol(-1) higher in free energy than the native state under non-denaturing conditions at neutral pH. The partially folded intermediate is characterized as having an unfolded N-terminal subdomain while the C-terminal subdomain retains a native-like fold. Although the majority of the residues in the N-terminal subdomain sample a random-coil distribution of conformations, deviations of backbone amide 1H and 15N chemical shifts from canonical random-coil values for residues within 5A of the His41 imidazole ring indicate that a significant degree of residual structure is maintained in the partially folded ensemble. The pH-dependence of exchange broadening is consistent with a linear three-state exchange model whereby unfolding of the N-terminal subdomain is coupled to titration of His41 in the partially folded intermediate with a pKa,I=5.69+/-0.07. Although maintenance of residual interactions with the imidazole ring in the unfolded N-terminal subdomain appears to reduce pKa,I compared to model histidine compounds, protonation of His41 disrupts these interactions and reduces the difference in free energy between the native state and partially folded intermediate under acidic conditions. In addition, chemical shift changes for residues Lys70-Phe76 in the C-terminal subdomain suggest that the HP67 actin binding site is disrupted upon unfolding of the N-terminal subdomain, providing a potential mechanism for regulating the villin-dependent bundling of actin filaments.

Conformational studies of a hyperthermostable enzyme

The structural features of the hyperthermophilic endo-beta-1,3-glucanase from Pyrococcus furiosus were studied using circular dichroism, steady-state and time-resolved fluorescence spectroscopy and anisotropy. Upon heat and chemical treatment the folded and denatured states of the protein were characterized by distinguishable spectral profiles that identified a number of conformational states. The fluorescence methods showed that the spectral differences arose from changes in the local environment around specific tryptophan residues in the native, partially folded, partially unfolded and completely unfolded state. A structural resemblance was observed between the native protein and the structurally perturbed state which resulted after heat treatment at 110 degrees C. The enzyme underwent disruption of the native secondary and tertiary structure only after incubation at biologically extremely high temperatures (i.e. 150 degrees C), whilst in the presence of 8 m of guanidine hydrochloride the protein was partially unfolded.

Mutational Analysis Demonstrates that Specific Electrostatic Interactions can Play a Key Role in the Denatured State Ensemble of Proteins

The nature of the denatured state ensemble has been controversial for decades owing, in large part, to the difficulty in characterizing the structure and energetics of denatured state interactions. There is increasing evidence for relatively non-specific hydrophobic clustering in the denatured states of some proteins but other types of interactions are much less well characterized. Here, we report the characterization of highly specific electrostatic interactions in the denatured state of a small alpha-beta protein, the N-terminal domain of the ribosomal protein L9 (NTL9). Mutation of Lys12 to Met has been shown to increase the stability of NTL9 significantly through the disruption of denatured state interactions. Here, we describe the analysis of the pH-dependent stability of 13 mutants designed to probe the nature of the Lys12 denatured state interaction. Lys12 is located in a lysine-rich region of the protein but analysis of a set of Lys to Met mutants shows that it plays a unique role in the denatured state. Analysis of mutants of all of the acidic residues in NTL9 shows that Lys12 forms a specific non-native electrostatic interaction with Asp8 in the denatured state ensemble. Thus the distribution of charge-charge interactions in the denatured state ensemble of NTL9 appears to be biased by few key interactions and is very different from that expected in a random coil. We propose that these interactions are not encoded by local sequence effects but rather reflect interactions among residues more distant in sequence. These results demonstrate that electrostatic as well as hydrophobic interactions can play an important role in the denatured state ensemble.

Solution structure of a protein denatured state and folding intermediate

The most controversial area in protein folding concerns its earliest stages. Questions such as whether there are genuine folding intermediates, and whether the events at the earliest stages are just rearrangements of the denatured state or progress from populated transition states, remain unresolved. The problem is that there is a lack of experimental high-resolution structural information about early folding intermediates and denatured states under conditions that favour folding because competent states spontaneously fold rapidly. Here we have solved directly the solution structure of a true denatured state by nuclear magnetic resonance under conditions that would normally favour folding, and directly studied its equilibrium and kinetic behaviour. We engineered a mutant of Drosophila melanogaster Engrailed homeodomain that folds and unfolds reversibly just by changing ionic strength. At high ionic strength, the mutant L16A is an ultra-fast folding native protein, just like the wild-type protein; however, at physiological ionic strength it is denatured. The denatured state is a well-ordered folding intermediate, poised to fold by docking helices and breaking some non-native interactions. It unfolds relatively progressively with increasingly denaturing conditions, and so superficially resembles a denatured state with properties that vary with conditions. Such ill-defined unfolding is a common feature of early folding intermediate states and accounts for why there are so many controversies about intermediates versus compact denatured states in protein folding.

Influence of denatured and intermediate states of folding on protein aggregation

We simulate the aggregation thermodynamics and kinetics of proteins L and G, each of which self-assembles to the same alpha/beta [corrected] topology through distinct folding mechanisms. We find that the aggregation kinetics of both proteins at an experimentally relevant concentration exhibit both fast and slow aggregation pathways, although a greater proportion of protein G aggregation events are slow relative to those of found for protein L. These kinetic differences are correlated with the amount and distribution of intrachain contacts formed in the denatured state ensemble (DSE), or an intermediate state ensemble (ISE) if it exists, as well as the folding timescales of the two proteins. Protein G aggregates more slowly than protein L due to its rapidly formed folding intermediate, which exhibits native intrachain contacts spread across the protein, suggesting that certain early folding intermediates may be selected for by evolution due to their protective role against unwanted aggregation. Protein L shows only localized native structure in the DSE with timescales of folding that are commensurate with the aggregation timescale, leaving it vulnerable to domain swapping or nonnative interactions with other chains that increase the aggregation rate. Folding experiments that characterize the structural signatures of the DSE, ISE, or the transition state ensemble (TSE) under nonaggregating conditions should be able to predict regions where interchain contacts will be made in the aggregate, and to predict slower aggregation rates for proteins with contacts that are dispersed across the fold. Since proteins L and G can both form amyloid fibrils, this work also provides mechanistic and structural insight into the formation of prefibrillar species.

Comparison of Guanidine Hydrochloride (GdnHCl) and Urea Denaturation on Inactivation and Unfolding of Human Placental Cystatin (HPC)

The activity and conformational change of human placental cystatin (HPC), a low molecular weight thiol proteinase inhibitor (12,500) has been investigated in presence of guanidine hydrochloride (GdnHCl) and urea. The denaturation of HPC was followed by activity measurements, fluorescence spectroscopy and Circular Dichroism (CD) studies. Increasing the denaturant concentration significantly enhanced the inactivation and unfolding of HPC. The enzyme was 50% inactivated at 1.5 M GdnHCl or 3 M urea. Up to 1.5 M GdnHCl concentration there was quenching of fluorescence intensity compared to native form however at 2 M concentration intensity increased and emission maxima had 5 nm red shift with complete unfolding in 4-6 M range. The mid point of transition was in the region of 1.5-2 M. In case of urea denaturation, the fluorescence intensity increased gradually with increase in the concentration of denaturant. The protein unfolded completely in 6-8 M concentration of urea with a mid-point of transition at 3 M. CD spectroscopy shows that the ellipticity of HPC has increased compared to that of native up to 1.5 M GdnHCl and then there is gradual decrease in ellipticity from 2 to 5 M concentration. At 6 M GdnHCl the protein had random coil conformation. For urea the ellipticity decreases with increase in concentration showing a sigmoidal shaped transition curve with little change up to 1 M urea. The protein greatly loses its structure at 6 M urea and at 8 M it is a random coil. The urea induced denaturation follows two-state rule in which Native-->Denatured state transition occurs in a single step whereas in case of GdnHCl, intermediates or non-native states are observed at lower concentrations of denaturant. These intermediate states are possibly due to stabilizing properties of guanidine cation (Gdn+) at lower concentrations, whereas at higher concentrations it acts as a classical denaturant.

Recent developments in structural proteomics for protein structure determination

The major challenges in structural proteomics include identifying all the proteins on the genome-wide scale, determining their structure-function relationships, and outlining the precise three-dimensional structures of the proteins. Protein structures are typically determined by experimental approaches such as X-ray crystallography or nuclear magnetic resonance (NMR) spectroscopy. However, the knowledge of three-dimensional space by these techniques is still limited. Thus, computational methods such as comparative and de novo approaches and molecular dynamic simulations are intensively used as alternative tools to predict the three-dimensional structures and dynamic behavior of proteins. This review summarizes recent developments in structural proteomics for protein structure determination; including instrumental methods such as X-ray crystallography and NMR spectroscopy, and computational methods such as comparative and de novo structure prediction and molecular dynamics simulations.

Direct characterization of the folded, unfolded and urea-denatured states of the C-terminal domain of the ribosomal protein L9

The stability of the isolated C-terminal domain of the ribosomal protein L9 (CTL9) is strongly dependent upon pH. Below pH 4.2, the folded and unfolded states are both populated significantly. Their interconversion is slow on the NMR chemical shift time-scale and separate, well-resolved resonances from each state are observed. This allows the hydrodynamic properties of both states to be studied under identical conditions by using pulse field gradient NMR experiments. Hydrodynamic radii of the folded, unfolded and urea denatured protein molecules at pD 3.8 have been derived. The acid-denatured protein has a significantly smaller hydrodynamic radius, 28.2A, compared to that of the urea-denatured protein, which is 33.6A at pD 3.8. Far-UV CD spectra show that there is more residual secondary structure retained in the acid-denatured ensemble than in the urea-denatured one. ANS binding experiments and analysis of the CD data show that this acid-denatured species is not a molten globule state. Diffusion measurements of CTL9 were conducted over the pD range from 2.1 to 7.0. The hydrodynamic radii of both the folded and the acid-unfolded protein start to increase below pD 4, with the radius of hydration of the acid-unfolded state increasing from 25.1A at pD 4.2 to 33.5A at pD 2.1. The hydrodynamic radius of the urea-denatured protein is much less sensitive to pH. The unfolded protein at pD 2.1, no urea, has almost the same hydrodynamic radius as the urea-denatured protein at pD 3.8. The CD spectra, however, show significant differences in residual secondary structure, and the acid-denatured state contains more structure.

Formation of Native and Non-native Interactions in Ensembles of Denatured ACBP Molecules from Paramagnetic Relaxation Enhancement Studies

Paramagnetic relaxation enhancement measurements in the denatured state of ACBP have provided distance restraints that have been used in computer simulations to determine the conformational ensembles representing the denatured states of ACBP under a variety of conditions. A detailed comparison of the residual structure in the denatured state of ACBP under these different conditions has enabled us to infer that regions in the N and C-terminal parts of the protein sequence have a high tendency to interact in the unfolded state under physiological conditions. By comparing the structural features in the denatured states with those in the transition state for folding we also provided new insights into the mechanism of formation of the native state of this protein.

Conformational Distribution of a 14-Residue Peptide in Solution: A Fluorescence Resonance Energy Transfer Study

We demonstrate here that a nitrile-derivatized phenylalanine residue, p-cyanophenylalanine (Phe(CN)), and tryptophan (Trp) constitute a novel donor-acceptor pair for fluorescence resonance energy transfer (FRET). The Förster distance of this FRET pair was determined to be approximately 16 A and hence is well suited for determining relatively short separation distances. To validate the applicability of this FRET pair in conformational studies, we studied the conformational heterogeneity of a 14-residue amphipathic peptide, Mastoparan X (MPx peptide), in water and 7 M urea solution as well as at different temperatures. Specifically, seven nitrile-derivatized mutants of the MPx peptide, each containing a Phe(CN) residue that replaces different positions along the peptide sequence (i.e., from position 5 to 11) and serves as a resonance energy donor to the native Trp residue at position 3, were studied spectroscopically. The FRET efficiencies obtained from these peptides allowed us to gain a global picture regarding the conformational distribution of the MPx peptide in different environments. Our results suggest that the MPx molecules exist in water as an ensemble of rather compact conformations, with a radius of gyration of approximately 4.2 A, whereas in 7 M urea the radius of gyration increases to approximately 6.5 A, indicating that the peptide conformations become more extended under this condition. However, we found that temperature had only a negligible effect on the size of the MPx peptide, underlining the difference between the thermally and chemically denatured states of polypeptides. The application of the Gaussian chain or the wormlike chain model allowed us to further obtain the probability distribution function of the separation distance between any two residues along the peptide sequence. We found that the effective bond length of the MPx peptide, obtained by using the Gaussian chain model, is 2.78 A in water and 4.28 A in 7 M urea.

Unassisted refolding of urea-denatured arginine kinase from shrimp Feneropenaeus chinensis: evidence for two equilibrium intermediates in the refolding pathway

The refolding process and the equilibrium intermediates of urea-denatured arginine kinase (AK) were investigated by 1-anilino-8-naphthalenesulfonate (ANS) intrinsic fluorescence, far-UV circular dichroism (CD), size-exclusion chromatography (SEC), and enzymatic activity. In dilute denaturant, two equilibrium refolding intermediates (I and N') were discovered, and a refolding scheme of urea-denatured AK was proposed. During the refolding of urea-denatured AK, the fluorescence intensity increased remarkably, accompanied by a significant blue shift of the emission maximum and a pronounced increase in molar ellipticity of CD at 222 nm. The first folding intermediate (I) was inactive in urea solution ranging between 2.4 and 3.0 M. The second (N') existed between a 0.4- and 0.8-M urea solution, with slightly increased activity. Neither the blue shift emission maximum nor the molar ellipticity of CD at 222 nm showed significant changes in these two regions. The two intermediates were characterized by monitoring the ANS binding ability in various residual urea solutions, and two peaks of the emission intensity were observed in urea solutions of 0.6 and 2.8 M, respectively. The SEC results indicated that a distribution coefficient (K(D)) platform existed in urea solutions ranging between 2.4 and 3.0 M urea, suggesting that there was a similarly apparent protein profile and size in the urea solution region. The refolding kinetics showed that the urea-denatured AK was in two-phase refolding. Proline isomerization occurred in the unfolding process of AK, which blocked the slow phase of refolding. These results suggested that the refolding process of urea-denatured AK contained at the least two equilibrium refolding intermediates.

Native and nonnative conformational preferences in the urea-unfolded state of barstar

The refolding of barstar from its urea-unfolded state has been studied extensively using various spectroscopic probes and real-time NMR, which provide global and residue-specific information, respectively, about the folding process. Here, a preliminary structural characterization by NMR of barstar in 8 M urea has been carried out at pH 6.5 and 25 degrees C. Complete backbone resonance assignments of the urea-unfolded protein were obtained using the recently developed three-dimensional NMR techniques of HNN and HN(C)N. The conformational propensities of the polypeptide backbone in the presence of 8 M urea have been estimated by examining deviations of secondary chemical shifts from random coil values. For some residues that belong to helices in native barstar, 13C(alpha) and 13CO secondary shifts show positive deviations in the urea-unfolded state, indicating that these residues have propensities toward helical conformations. These residues are, however, juxtaposed by residues that display negative deviations indicative of propensities toward extended conformations. Thus, segments that are helical in native barstar are unlikely to preferentially populate the helical conformation in the unfolded state. Similarly, residues belonging to beta-strands 1 and 2 of native barstar do not appear to show any conformational preferences in the unfolded state. On the other hand, residues belonging to the beta-strand 3 segment show weak nonnative helical conformational preferences in the unfolded state, indicating that this segment may possess a weak preference for populating a helical conformation in the unfolded state.

Disorder in a target for the smad2 mad homology 2 domain and its implications for binding and specificity

The Smad2 Mad homology 2 (MH2) domain binds to a diverse group of proteins which do not share a common sequence motif. We have used NMR to investigate the structure of one of these interacting proteins, the Smad binding domain (SBD) of Smad anchor for receptor activation (SARA). Our results indicate that the unbound SBD is highly disordered and forms no stable secondary or tertiary structures. Additionally we have used fluorescence binding studies to study the interaction between the MH2 domain and SBD and find that no region of the SBD dominates the interaction between the MH2 and the SBD. Our results are consistent with a series of hydrophobic patches on the MH2 that are able to recognize disordered regions of proteins. These findings elucidate a mechanism by which a single domain (MH2) can specifically recognize a diverse set of proteins which are unrelated by sequence, lead to a clearer picture of how MH2 domains function in the transforming growth factor-beta-signaling pathway and suggest possible mechanisms for controlling interactions with MH2 domains.

Absence of kinetic thermal stabilization in a hyperthermophile rubredoxin indicated by 40 microsecond folding in the presence of irreversible denaturation

The striking kinetic stability of many proteins derived from hyperthermophilic organisms has led to the proposal that such stability may result from a heightened activation barrier for unfolding independent of a corresponding increase in the thermodynamic stability. This in turn implies a corresponding retardation of the folding reaction. A commonly cited model for kinetic thermal stabilization is the rubredoxin from Pyrococcus furiosus (Pf), which exhibits an irreversible denaturation lifetime at 100 degrees C of nearly a week. Utilizing protein resonances shifted well outside of the random coil chemical shift envelope, nuclear magnetic resonance (NMR) chemical exchange measurements on Pf rubredoxin as well as on the mesophile Clostridium pasteurianum (Cp) rubredoxin demonstrate reversible thermal transition temperatures of 144 degrees C (137 degrees C for the N-terminal modified A2K variant) and 104 degrees C, respectively, with similar (un)folding rates of approximately 25,000 s(-1), only modestly slower than the diffusion controlled rate. The absence of a substantial activation barrier to rubredoxin folding as well as the similar folding kinetics of the mesophile protein indicate that kinetic stabilization has not been utilized by the hyperthermophile rubredoxin in achieving its extreme thermal stability. The two-state folding kinetics observed for Pf rubredoxin contradict a previous assertion of multiphasic folding based on hydrogen exchange data extrapolated to an estimated midpoint of transition temperature (T(m)) of nearly 200 degrees C. This discrepancy is resolved by the observation that the base-catalyzed hydrogen exchange of the model dipeptide (N-acetyl-L-cysteine-N-methylamide)4-Cd2+ is 23-fold slower than that of the free cysteine model dipeptide used to normalize the Pf rubredoxin hydrogen exchange data.

Conformational Properties of the Iso-1-Cytochrome c Denatured State: Dependence on Guanidine Hydrochloride Concentration

Production of seven single surface histidine variants of yeast iso-1-cytochrome c allowed measurement of the apparent pK(a), pK(a)(obs), for histidine-heme loop formation for loops of nine to 83 amino acid residues under varying denaturing conditions (2 M to 6 M guanidine hydrochloride, gdnHCl). A linear correlation between pK(a)(obs) and the log of the loop size is expected for a random coil, pK(a)(obs) proportional to k log(n), where k is a scaling factor and n is the number of monomers in the loop. For small loops of nine, 16, and 22 monomers, no dependence of pK(a)(obs) on loop size was observed at any denaturant concentration indicating effects from chain stiffness. For larger loops of 37, 56, 72, and 83 monomers, the dependence of pK(a)(obs) on log(n) was linear and the slope of that dependence decreased with increasing concentration of denaturant. The scaling factor obtained at 5 M and 6 M gdnHCl for the larger loop sizes was approximately -2.0, close to the value of -2.2 expected for a random coil with excluded volume. However, scaling factors obtained under less harsh denaturing conditions (2 M to 4.5 M gdnHCl) deviated strongly from that expected for a random coil, being in the range -3 to -4. The gdnHCl dependence of pK(a)(obs) at each loop size was also evaluated to obtain denaturant m-values. Short loops where chain stiffness dominates had similar m-values of approximately 0.25 kcal/mol M. For larger loops m-values decrease with increasing loop size indicating that less hydrophobic area is sequestered when larger loops form. It is known that the earliest events in protein folding involve the formation of simple loops. The data from these studies provide direct insight into the relative probability with which loops of different sizes will form, as well as the factors which affect loop formation.

Five Hierarchical Levels of Sequence-Structure Correlation in Proteins

This article reviews recent work towards modelling protein folding pathways using a bioinformatics approach. Statistical models have been developed for sequence-structure correlations in proteins at five levels of structural complexity: (i) short motifs; (ii) extended motifs; (iii) nonlocal pairs of motifs; (iv) 3-dimensional arrangements of multiple motifs; and (v) global structural homology. We review statistical models, including sequence profiles, hidden Markov models (HMMs) and interaction potentials, for the first four levels of structural detail. The I-sites (folding Initiation sites) Library models short local structure motifs. Each succeeding level has a statistical model, as follows: HMMSTR (HMM for STRucture) is an HMM for extended motifs; HMMSTR-CM (Contact Maps) is a model for pairwise interactions between motifs; and SCALI-HMM (HMMs for Structural Core ALIgnments) is a set of HMMs for the spatial arrangements of motifs. The parallels between the statistical models and theoretical models for folding pathways are discussed in this article; however, global sequence models are not discussed because they have been extensively reviewed elsewhere. The data used and algorithms presented in this article are available at http://www.bioinfo.rpi.edu/~bystrc/ (click on "servers" or "downloads") or by request to bystrc@rpi.edu .

The denatured state of Engrailed Homeodomain under denaturing and native conditions

Protein folding starts from the elusive form of the denatured state that is present under conditions that favour the native state. We have studied the denatured state of Engrailed Homeodomain (En-HD) under mildly and strongly denaturing conditions at the level of individual residues by NMR and more globally by conventional spectroscopy and solution X-ray scattering. We have compared these states with a destabilized mutant, L16A, which is predominantly denatured under conditions where the wild-type is native. This engineered denatured state, which could be directly studied under native conditions, was in genuine equilibrium with the native state, which could be observably populated by changing the conditions or introducing a stabilizing mutation. The denatured state had extensive native secondary structure and was significantly compact and globular. But, the side-chains and backbone were highly mobile. Non-cooperative melting of the residual structure on the denatured state of En-HD was observed, both at the residue and the molecular level, with increasingly denaturing conditions. The absence of a co-operative transition could result from the denatured state ensemble progressing through a series of intermediates or from a more general slide (second-order transition) from the compact form under native conditions to the more extended at highly denaturing conditions. In either case, the starting point for folding under native conditions is highly structured and already poised to adopt the native structure.

The relationship between conservation, thermodynamic stability, and function in the SH3 domain hydrophobic core

To investigate the relationships between sequence conservation, protein stability, and protein function, we have measured the thermodynamic stability, folding kinetics, and in vitro peptide-binding activity of a large number of single-site substitutions in the hydrophobic core of the Fyn SH3 domain. Comparison of these data to that derived from an analysis of a large alignment of SH3 domain sequences revealed a very good correlation between the distinct pattern of conservation observed at each core position and the thermodynamic stability of mutants. Conservation was also found to correlate well with the unfolding rates of mutants, but not to the folding rates, suggesting that evolution selects more strongly for optimal native state packing interactions than for maximal folding rates. Structural analysis suggests that residue-residue core packing interactions are very similar in all SH3 domains, which provides an explanation for the correlation between conservation and mutant stability effects studied in a single SH3 domain. We also demonstrate a correlation between stability and the in vivo activity of mutants, and between conservation and activity. However, the relationship between conservation and activity was very strong only for the three most conserved hydrophobic core positions. The weaker correlation between activity and conservation seen at the other seven core positions indicates that maintenance of protein stability is the dominant selective pressure at these positions. In general, the pattern of conservation at hydrophobic core positions appears to arise from conserved packing constraints, and can be effectively utilized to predict the destabilizing effects of amino acid substitutions.

Structural correspondence between the alpha-helix and the random-flight chain resolves how unfolded proteins can have native-like properties

Recently, we have proposed that, on average, the structure of the unfolded state of small, mostly alpha-helical proteins may be similar to the native structure (the 'mean-structure' hypothesis). After examining thousands of simulations of both the folded and the unfolded states of five polypeptides in atomistic detail at room temperature, we report here a result that seems at odds with the mean-structure hypothesis. Specifically, the average inter-residue distances in the collapsed unfolded structures agree well with the statistics of the ideal random-flight chain with link length of 3.8 A (the length of one amino acid). A possible resolution of this apparent contradiction is offered by the observation that the inter-residue distances in a typical alpha-helix over short stretches are close to the average distances in an ideal random-flight chain.

Folding subdomains of thioredoxin characterized by native-state hydrogen exchange

Native-state hydrogen exchange (HX) studies, used in conjunction with NMR spectroscopy, have been carried out on Escherichia coli thioredoxin (Trx) for characterizing two folding subdomains of the protein. The backbone amide protons of only the slowest-exchanging 24 amino acid residues, of a total of 108 amino acid residues, could be followed at pH 7. The free energy of the opening event that results in an amide hydrogen exchanging with solvent (DeltaG(op)) was determined at each of the 24 amide hydrogen sites. The values of DeltaG(op) for the amide hydrogens belonging to residues in the helices alpha(1), alpha(2), and alpha(4) are consistent with them exchanging with the solvent only when the fully unfolded state is sampled transiently under native conditions. The denaturant-dependences of the values of DeltaG(op) provide very little evidence that the protein samples partially unfolded forms, lower in energy than the unfolded state. The amide hydrogens belonging to the residues in the beta strands, which form the core of the protein, appear to have higher values of DeltaG(op) than amide hydrogens belonging to residues in the helices, suggesting that they might be more stable to exchange. This apparently higher stability to HX of the beta strands might be either because they exchange out their amide hydrogens in a high energy intermediate preceding the globally unfolded state, or, more likely, because they form residual structure in the globally unfolded state. In either case, the central beta strands-beta(3,) beta(2), and beta(4)-would appear to form a cooperatively folding subunit of the protein. The native-state HX methodology has made it possible to characterize the free energy landscape that Trx can sample under equilibrium native conditions.

Posttransition state desolvation of the hydrophobic core of the src-SH3 protein domain

The folding thermodynamics of the src-SH3 protein domain were characterized under refolding conditions through biased fully atomic molecular dynamics simulations with explicit solvent. The calculated free energy surfaces along several reaction coordinates revealed two barriers. The first, larger barrier was identified as the transition state barrier for folding, associated with the formation of the first hydrophobic sheet of the protein. phi values calculated from structures residing at the transition state barrier agree well with experimental phi values. The microscopic information obtained from our simulations allowed us to unambiguously assign intermediate phi values as the result of multiple folding pathways. The second, smaller barrier occurs later in the folding process and is associated with the cooperative expulsion of water molecules between the hydrophobic sheets of the protein. This posttransition state desolvation barrier cannot be observed through traditional folding experiments, but is found to be critical to the correct packing of the hydrophobic core in the final stages of folding. Hydrogen exchange and NMR experiments are suggested to probe this barrier.

Site-specific contributions to the pH dependence of protein stability

Understanding protein stability is a significant challenge requiring characterization of interactions within both folded and unfolded states. Of these, electrostatic interactions influence ionization equilibria of acidic and basic groups and diversify their pK(a) values. The pH dependence of the thermodynamic stability (Delta G(FU)) of a protein arises as a consequence of differential pK(a) values between folded and unfolded states. Previous attempts to calculate pH-dependent contributions to stability have been limited by the lack of experimental unfolded state pK(a) values. Using recently developed NMR spectroscopic methods, we have determined residue-specific pK(a) values for a thermodynamically unstable Src homology 3 domain in both states, enabling the calculation of the pH dependence of stability based on simple analytical expressions. The calculated pH stability profile obtained agrees very well with experiment, unlike profiles derived from two current models of electrostatic interactions within unfolded states. Most importantly, per-residue contributions to the pH dependence of Delta G(FU) derived from the data provide insights into specific electrostatic interactions in both the folded and unfolded states and their roles in protein stability. These interactions include a hydrogen bond between the Asp-8 side-chain and the Lys-21 backbone amide group in the folded state, which represents a highly conserved interaction in Src homology 3 domains.

Folding of a highly conserved diverging turn motif from the SH3 domain

Recent NMR structural characterization studies showed that a seven-residue segment (FKKGERL) from the src SH3 domain adopts the nativelike diverging type II beta-turn in aqueous solution in support of the prediction based on the I-sites library of sequence structural motifs. We study the conformational variability and folding/unfolding thermodynamics of this peptide in explicit solvent using replica-exchange molecular dynamics simulations, which greatly enhances the sampling of the conformational space. This peptide samples three main free energy basins (nativelike, intermediate, and unfolded) separated by small barriers. The nativelike basin is fractionally populated (DeltaG(300K) = 0.4 kcal/mol) with structures that satisfy a subset of the NMR-derived constraints. The intrinsic stability of the diverging turn is examined in relationship to the nature of three specific contacts: a turn-hydrogen bond, a mainchain-to-sidechain hydrogen bond, and an end-to-end hydrophobic contact. We have carried out simulations of mutants at the highly conserved GE positions in the sequence. The mutation E5D destabilizes the isolated diverging turn motif, contrary to the observation that this mutation stabilizes the fyn SH3 domain. The G4T mutation also destabilizes the isolated diverging turn; however, the extent of destabilization is smaller than that of the reverse mutation in the drk SH3.

Residual charge interactions in unfolded staphylococcal nuclease can be explained by the Gaussian-chain model

The discrepancy of the pH dependence of the unfolding free energy for staphylococcal nuclease from what is expected from an idealized model for the unfolded state is accounted for by the recently developed Gaussian-chain model. Residual electrostatic effects in the unfolded state are attributed to nonspecific interactions dominated by charges close along the sequence. The dominance of nonspecific local interactions appears to be supported by some experimental evidence.

Mechanism of fast protein folding

An explosion of in vitro experimental data on the folding of proteins has revealed many examples of folding in the millisecond or faster timescale, often occurring in the absence of stable intermediate states. We review experimental methods for measuring fast protein folding kinetics, and then discuss various analytical models used to interpret these data. Finally, we classify general mechanisms that have been proposed to explain fast protein folding into two catagories, heterogeneous and homogeneous, reflecting the nature of the transition state. One heterogeneous mechanism, the diffusion-collision mechanism, can be used to interpret experimental data for a number of proteins.

Transient structure formation in unfolded acyl-coenzyme A-binding protein observed by site-directed spin labelling

Paramagnetic relaxation has been used to monitor the formation of structure in the folding peptide chain of guanidinium chloride-denatured acyl-coenzyme A-binding protein. The spin label (1-oxyl-2,2,5,5-tetramethyl-3-pyrroline-3-methyl)methanesulfonate (MTSL) was covalently bound to a single cysteine residue introduced into five different positions in the amino acid sequence. It was shown that the formation of structure in the folding peptide chain at conditions where 95% of the sample is unfolded brings the relaxation probe close to a wide range of residues in the peptide chain, which are not affected in the native folded structure. It is suggested that the experiment is recording the formation of many discrete and transient structures in the polypeptide chain in the preface of protein folding. Analysis of secondary chemical shifts shows a high propensity for alpha-helix formation in the C-terminal part of the polypeptide chain, which forms an alpha-helix in the native structure and a high propensity for turn formation in two regions of the polypeptide that form turns in the native structure. The results contribute to the idea that native-like structural elements form transiently in the unfolded state, and that these may be of importance to the initiation of protein folding.

Native-like mean structure in the unfolded ensemble of small proteins

The nature of the unfolded state plays a great role in our understanding of proteins. However, accurately studying the unfolded state with computer simulation is difficult, due to its complexity and the great deal of sampling required. Using a supercluster of over 10,000 processors we have performed close to 800 micros of molecular dynamics simulation in atomistic detail of the folded and unfolded states of three polypeptides from a range of structural classes: the all-alpha villin headpiece molecule, the beta hairpin tryptophan zipper, and a designed alpha-beta zinc finger mimic. A comparison between the folded and the unfolded ensembles reveals that, even though virtually none of the individual members of the unfolded ensemble exhibits native-like features, the mean unfolded structure (averaged over the entire unfolded ensemble) has a native-like geometry. This suggests several novel implications for protein folding and structure prediction as well as new interpretations for experiments which find structure in ensemble-averaged measurements.

Cooperative interactions and a non-native buried Trp in the unfolded state of an SH3 domain

The presence of residual structure in the unfolded state of the N-terminal SH3 domain of Drosophila drk (drkN SH3 domain) has been investigated using far- and near-UV circular dichroism (CD), fluorescence, and NMR spectroscopy. The unfolded (U(exch)) state of the drkN SH3 domain is significantly populated and exists in equilibrium with the folded (F(exch)) state under non-denaturing conditions near physiological pH. Denaturation experiments have been performed on the drkN SH3 domain in order to monitor the change in ellipticity, fluorescence intensity, and chemical shift between the U(exch) state and chemically or thermally denatured states. Differences between the unfolded and chemically or thermally denatured states highlight specific areas of residual structure in the unfolded state that are cooperatively disrupted upon denaturation. Results provide evidence for cooperative interactions in the unfolded state involving residues of the central beta-sheet, particularly the beta4 strand. Denaturation as well as hydrogen-exchange experiments demonstrate a non-native burial of the Trp ring within this "cooperative" core of the unfolded state. These findings support the presence of non-native hydrophobic clusters, organised by Trp rings, within disordered states.

An NMR view of the folding process of a CheY mutant at the residue level

The folding of CheY mutant F14N/V83T was studied at 75 residues by NMR. Fluorescence, NMR, and sedimentation equilibrium studies at different urea and protein concentrations reveal that the urea-induced unfolding of this CheY mutant includes an on-pathway molten globule-like intermediate that can associate off-pathway. The populations of native and denatured forms have been quantified from a series of 15N-1H HSQC spectra recorded under increasing concentrations of urea. A thermodynamic analysis of these data provides a detailed picture of the mutant's unfolding at the residue level: (1) the transition from the native state to the molten globule-like intermediate is highly cooperative, and (2) the unfolding of this state is sequential and yields another intermediate showing a collapsed N-terminal domain and an unfolded C-terminal tail. This state presents a striking similarity to the kinetic transition state of the CheY folding pathway.