Cold denaturation and heat denaturation of Streptomyces subtilisin inhibitor. 2. 1H NMR studies

Structural transitions of the protein Streptomyces subtilisin inhibitor (SSI) from the native state to the cold-denatured and heat-denatured states were studied by 1H NMR spectroscopy in the temperature range from -10 to 60 degrees C in the acidic pH range. Assignments of some of the 1H NMR signals of SSI in the cold-denatured and heat-denatured states were performed by a combined use of selective deuteration and site-directed mutagenesis. Throughout the pH range from 2.1 to 3.1, both transitions were cooperative and basically only three distinct spectra corresponding to structures in the cold-denatured, native, and heat-denatured states were detected. In the cold-denatured state, the side-chain signals of Met73, His106, at least one Val, and two Leu were observed at distinctly shifted positions from those for a random-coiled structure, suggesting the formation of a tertiary structure, while those of Met70, His43, and Ala2 were observed at positions for a random-coiled structure. This tertiary structure in the cold-denatured state is entirely different from that in the native state, as some amino acid residues exposed to the solvent in the native state (e.g., Met73, His106) are buried while those sequestered in the native state (e.g., His43) are exposed. In the heat-denatured state, however, most 1H NMR signals were observed at random-coiled positions, indicating that there is much less tertiary structure in the heat-denatured state than in the cold-denatured state. At pH values below 2.09, a structural transition was observed from the cold-denatured state to the heat-denatured state without passing through the native state.(ABSTRACT TRUNCATED AT 250 WORDS)     

Native-like beta-hairpin retained in the cold-denatured state of bovine beta-lactoglobulin.

Bovine beta-lactoglobulin is denatured by increased temperature (heat denaturation) and by decreased temperature (cold-denaturation) in the presence of 4 M urea at pH 2.5. We characterized the structure of the cold-denatured state of beta-lactoglobulin using circular dichroism (CD), small-angle X-ray scattering (SAXS) and heteronuclear nuclear magnetic resonance (NMR). CD and SAXS indicated that the cold-denatured state, in comparison with the highly denatured state induced by urea, is rather compact, retaining some secondary structure, but no tertiary structure. The location of the residual structures in the cold-denatured state and their stability were characterized by 1H/2H exchange combined with heteronuclear NMR. The results indicated that the residues adjacent to the disulfide bond (C106-C119) connecting beta-strands G and H had markedly high protection factors, suggesting the presence of a native-like beta-hairpin stabilized by the disulfide bond. Since this beta-hairpin is conserved between different conformational states, including the kinetic refolding intermediate, it should be of paramount importance for the folding and stability of beta-lactoglobulin. On the other hand, the non-native alpha-helix suggested for the folding intermediate was not detected in the cold-denatured state. The 1H/2H exchange experiments showed that the protection factors of a mixture of the native and cold-denatured states is strongly biased by that of the labile cold-denatured state, consistent with a two-process model of the exchange.     

Helical and expanded conformation of equine beta-lactoglobulin in the cold-denatured state

The thermal unfolding transition of equine beta-lactoglobulin (ELG) was investigated by circular dichroism (CD) over a temperature range of -15 degrees C to 85 degrees C. In the presence of 2 M urea, a cooperative unfolding transition was observed both with increasing and decreasing temperature. The CD spectrum indicated that the heat and cold-denatured states of ELG have substantial secondary structures but lack persistent tertiary packing of the side-chains. In order to clarify the relation between the heat or cold-denatured state and the acid-denatured (A) state characterized previously, we have attempted to observe the temperature dependence of the CD spectrum at pH 1.5. The CD spectrum in the heat-denatured state is similar to that in the A state. The CD spectrum in the A state does not change cooperatively with increasing temperature. These results indicate that the heat-denatured state and the A state are the same structural state. On the other hand, the CD intensity at acid pH cooperatively increased with decreasing temperature. The CD spectrum at low temperature and acid pH is consistent with that in the cold-denatured state. Therefore, the cold-denatured state is distinguished from the heat-denatured state or the A state, and ELG assumes a larger amount of non-native alpha-helices in the cold-denatured state. Small angle X-ray scattering and analytical ultracentrifugation have indicated that ELG assumes an expanded chain-like conformation in the cold-denatured state in contrast to the compact globular conformation in the A state. The relation between the molecular size and the helical content in the partially folded states is discussed.     

Urea-induced conformational changes in cold- and heat-denatured states of a protein, Streptomyces subtilisin inhibitor.

Streptomyces subtilisin inhibitor (SSI) is known to exist in at least two distinct denatured states, cold-denatured (D') and heat-denatured (D) under acidic conditions. In the present work, we investigated the manner how increasing urea concentration from 0 to 8 M changes the polypeptide chain conformation of SSI that exists initially in the D' and D states as well as in the native state (N), in terms of the secondary structure, the tertiary structure, and the chain form, based on the results of the experiments using circular dichroism (CD), small-angle X-ray scattering (SAXS) and 1H-NMR spectroscopy. Our results indicate that the urea-induced conformational transitions of SSI under typical conditions of D' (pH 1.8, 3 degrees C) occur at least in two steps. In the urea concentration range of 0-2 M (step 1), a cooperative destruction of the tertiary structure occurs, resulting in a mildly denatured state (DU), which may still contain a little amount of secondary structures. In the concentration range of 2-4 M urea (step 2), the DU state gradually loses its residual secondary structure, and increases the radius of gyration nearly to a maximum value. At 4 M urea, the polypeptide chain is highly disordered with highly mobile side chains. Increasing the urea concentration up to 8 M probably results in the more highly denatured or alternatively the stiffer chain conformations. The conformational transition starting from the N state proceeds essentially the same way as in the above scheme in which D' is replaced with N. The conformational transition starting from the D state lacks step 1 because the D state contains no tertiary structures and is similar to the DU state. The fact that similar conformations are reached at urea concentrations above 2 M from different conformations of D', D, and N indicates that the effect of urea dominates in determining the polypeptide conformation of SSI in the denatured states rather than the pH and temperature.     

Temperature control for kinetic refolding of heat-denatured ovalbumin.

The folding of heat-denatured ovalbumin, a non-inhibitory serpin with a molecular size of 45 kDa, was examined. Ovalbumin was heat-denatured at 80 degrees C under nonreducing conditions at pH 7.5 and then cooled either slowly or rapidly. Slow cooling allowed the heat-denatured ovalbumin to refold to its native structure with subsequent resistance to digestion by trypsin. Upon rapid cooling, by contrast, the heat-denatured molecules assumed the metastable non-native conformations that were susceptible to trypsin. The non-native species were marginally stable for several days at a low temperature, but the molecules were transformed slowly into the native conformation. Considering data from size-exclusion chromatography and from analyses of CD, intrinsic tryptophan fluorescence, and adsorption of the dye 1-anilinonaphthalene-8-sulfonate, we postulated that the non-native species that accumulated upon rapid cooling were compact but structureless globules with disordered side chains collectively as a folding intermediate. Temperature-jumped CD experiments revealed biphasic kinetics for the refolding process of heat-denatured ovalbumin, with the features of increasing and subsequently decreasing amplitude of the rapid and the slow phases, respectively, with the decrease in folding temperature. The temperature dependence of the refolding kinetics indicated that the yield of renaturation was maximal at about 55 degrees C. These findings suggested the kinetic partitioning of heat-denatured ovalbumin between alternative fates, slow renaturation to the native state and rapid collapse to the metastable intermediate state. Analysis of disulfide pairing revealed the formation of a scrambled form with non-native disulfide interactions in both the heat-denatured state and the intermediate state that accumulated upon rapid cooling, suggesting that non-native disulfide pairing is responsible for the kinetic barriers that retard the correct folding of ovalbumin.     

Effects of the difference in the unfolded-state ensemble on the folding of Escherichia coli dihydrofolate reductase

The unfolded state of a protein is an ensemble of a large number of conformations ranging from fully extended to compact structures. To investigate the effects of the difference in the unfolded-state ensemble on protein folding, we have studied the structure, stability, and folding of "circular" dihydrofolate reductase (DHFR) from Escherichia coli in which the N and C-terminal regions are cross-linked by a disulfide bond, and compared the results with those of disulfide-reduced "linear" DHFR. Equilibrium studies by circular dichroism, difference absorption spectra, solution X-ray scattering, and size-exclusion chromatography show that whereas the native structures of both proteins are essentially the same, the unfolded state of circular DHFR adopts more compact conformations than the unfolded state of the linear form, even with the absence of secondary structure. Circular DHFR is more stable than linear DHFR, which may be due to the decrease in the conformational entropy of the unfolded state as a result of circularization. Kinetic refolding measurements by stopped-flow circular dichroism and fluorescence show that under the native conditions both proteins accumulate a burst-phase intermediate having the same structures and both fold by the same complex folding mechanism with the same folding rates. Thus, the effects of the difference in the unfolded state of circular and linear DHFRs on the refolding reaction are not observed after the formation of the intermediate. This suggests that for the proteins with close termini in the native structure, early compaction of a protein molecule to form a specific folding intermediate with the N and C-terminal regions in close proximity is a crucial event in folding. If there is an enhancement in the folding reflecting the reduction in the breadth of the unfolded-state ensemble for circular DHFR, this acceleration must occur in the sub-millisecond time-range.     

Cold denaturation and heat denaturation of Streptomyces subtilisin inhibitor. 1. CD and DSC studies

Cold denaturation and heat denaturation of the protein Streptomyces subtilisin inhibitor (SSI) were studied in the pH range 1.84-3.21 and in the temperature range -3-70 degrees C by circular dichroism and scanning microcalorimetry. The native structure of the protein was apparently most stabilized at about 20 degrees C and was denatured upon heating and cooling from this temperature. Each denaturation was reversible and cooperative, proceeding in two-state transitions, that is, from the native state to the cold-denatured state or from the native state to the heat-denatured state. The two denatured states, however, were not perfect random-coiled structures, and they differed from each other, indicating that there exist three states in this temperature range, i.e., cold denatured, native, and heat denatured. The difference between the cold and heat denaturations was indicated first by circular dichroism. The isodichroic point for the transition from the native state to the cold-denatured state was different from that from the native state to the heat-denatured state in the pH range between 3.21 and 2.45. Moreover, molar ellipticity for the cold-denatured state was different from that of the heat-denatured state, and the transition from the former to the latter was observed at pH values below 2. Values of van't Hoff enthalpies from the native state to the heat-denatured state at pH values between 3.21 and 2.45 were obtained by curve fitting of the CD data, and delta Cp = 1.82 (+/- 0.11) [kcal/(mol.K)] was obtained from the linear plot of the enthalpies against temperature. The parameters obtained from the heat denaturation studies gave curves for delta G zero which were not in agreement with the experimental data in the cold denaturation region when extrapolated to the low temperature. Moreover, the value of the apparent delta Cp for the cold denaturation in the pH range 3.03-2.45 was estimated to be different from that for the heat denaturation, indicating that the mechanism of the cold denaturation of SSI is different from a simple cold denaturation.(ABSTRACT TRUNCATED AT 250 WORDS)     

Characterization of a common intermediate of pea lectin in the folding pathway induced by TFE and HFIP

When pea lectin was exposed to a low pH range, it was found that the secondary structure of the lectin resisted conformational changes to a large extent up to pH 2.4 and below this pH, a sharp transition was observed which could be due to the presence of 27 acidic amino acid residues present in the protein. The effects of 1,1,1,3,3,3 hexafluoro-isopropanol (HFIP) and 2,2,2-Trifluoroethanol (TFE) on the conformation of pea lectin at pH 2.4 were studied using circular dichroism and fluorescence spectroscopy. Analysis varying the TFE concentration showed that up to 80% TFE (v/v) protein retained the residual beta-structure accompanied by a loss in tertiary structure. A similar conformation is presumed to exist at 4% HFIP (v/v), with an increase in HFIP concentration structural rearrangements occurred and a transition from beta-structure to alpha-helical structure started from 12% HFIP which completed at 30% HFIP. Our studies show the occurrence of a common intermediate in the folding pathway of pea lectin induced by two different fluoroalcohols, which differ in their mode of action to stabilize the secondary structure of a given protein. While TFE was not found to induce any alpha-helical structure, HFIP caused the transition of pea lectin, which is predominantly a beta-sheet protein, to a structure rich in alpha-helical contacts. Thus, our results also point out the possibility of a non-hierarchical model of protein folding in lectins.     

Folding intermediates of a model three-helix bundle protein. Pressure and cold denaturation studies

The stability and equilibrium unfolding of a model three-helix bundle protein, alpha(3)-1, by guanidine hydrochloride (GdnHCl), hydrostatic pressure, and temperature have been investigated. The combined use of these denaturing agents allowed detection of two partially folded states of alpha(3)-1, as monitored by circular dichroism, intrinsic fluorescence emission, and fluorescence of the hydrophobic probe bis-ANS (4,4'-dianilino-1,1'-binaphthyl-5,5'-disulfonic acid). The overall free-energy change for complete unfolding of alpha(3)-1, determined from GdnHCl unfolding data, is +4.6 kcal/mol. The native state is stabilized by -1.4 kcal/mol relative to a partially folded pressure-denatured intermediate (I(1)). Cold denaturation at high pressure gives rise to a second partially (un)folded conformation (I(2)), suggesting a significant contribution of hydrophobic interactions to the stability of alpha(3)-1. The free energy of stabilization of the native-like state relative to I(2) is evaluated to be -2.5 kcal/mol. Bis-ANS binding to the pressure- and cold-denatured states indicates the existence of significant residual hydrophobic structure in the partially (un)folded states of alpha(3)-1. The demonstration of folding intermediates of alpha(3)-1 lends experimental support to a number of recent protein folding simulation studies of other three-helix bundle proteins that predicted the existence of such intermediates. The results are discussed in terms of the significance of de novo designed proteins for protein folding studies.     

Deceleration of Arginine Kinase Refolding by Induced Helical Structures

Arginine kinase (AK) is a key metabolic enzyme for keeping energy balance in invertebrates. Therefore, regulation of the enzymatic activity and the folding studies of AK from the various invertebrates have been the focus of investigation. We studied the effects of helical structures by using hexafluoroisopropanol (HFIP) on AK folding. Folding kinetic studies showed that the folding rates of the urea-denatured AKs were significantly decelerated after being induced in various concentrations of HFIP. AK lost its activity completely at concentrations greater than 60%. The results indicated that the HFIP-induced helical structures in the denatured state play a negative role in protein folding, and the helical structures induced in 5% (v/v) HFIP act as the most effective barrier against AK taking its native structure. The computational docking simulations (binding energies for −2.19 kcal/mol for AutoDock4.2 and −20.47 kcal/mol for Dock6.3) suggested that HFIP interacts with the several important residues that are predicted by both programs. The excessively pre-organized helical structures not only hampered the folding process, but also ultimately brought about changes in the three-dimensional conformation and biological function of AK.     

Beta-hairpin folding mechanism of a nine-residue peptide revealed from molecular dynamics simulations in explicit water

The beta-hairpin fold mechanism of a nine-residue peptide, which is modified from the beta-hairpin of alpha-amylase inhibitor tendamistat (residues 15-23), is studied through direct folding simulations in explicit water at native folding conditions. Three 300-nanosecond self-guided molecular dynamics (SGMD) simulations have revealed a series of beta-hairpin folding events. During these simulations, the peptide folds repeatedly into a major cluster of beta-hairpin structures, which agree well with nuclear magnetic resonance experimental observations. This major cluster is found to have the minimum conformational free energy among all sampled conformations. This peptide also folds into many other beta-hairpin structures, which represent some local free energy minimum states. In the unfolded state, the N-terminal residues of the peptide, Tyr-1, Gln-2, and Asn-3, have a confined conformational distribution. This confinement makes beta-hairpin the only energetically favored structure to fold. The unfolded state of this peptide is populated with conformations with non-native intrapeptide interactions. This peptide goes through fully hydrated conformations to eliminate non-native interactions before folding into a beta-hairpin. The folding of a beta-hairpin starts with side-chain interactions, which bring two strands together to form interstrand hydrogen bonds. The unfolding of the beta-hairpin is not simply the reverse of the folding process. Comparing unfolding simulations using MD and SGMD methods demonstrate that SGMD simulations can qualitatively reproduce the kinetics of the peptide system.     

The structure of precursor proteins during import into mitochondria

Precursor proteins must be at least partially unfolded during import into mitochondria, but their actual conformation during translocation is not known. Are proteins fully unfolded and threaded through the import machinery amino acid by amino acid, or do they retain some partial structure? The folding pathway of most proteins in vitro contains a partially folded intermediate known as the molten globule state, and it has been suggested that proteins are in the molten globule state during translocation across membranes. Here we show that precursors are normally fully unfolded during import into mitochondria. However, precursors containing residual structure can be imported, if less efficiently.     

Structure of an Unfolding Intermediate of an RRM Domain of ETR-3 Reveals Its Native-like Fold

Prevalence of one or more partially folded intermediates during protein unfolding with different secondary and ternary conformations has been identified as an integral character of protein unfolding. These transition-state species need to be characterized structurally for elucidation of their folding pathways. We have determined the three-dimensional structure of an intermediate state with increased conformational space sampling under urea-denaturing condition. The protein unfolds completely at 10 M urea but retains residual secondary structural propensities with restricted motion. Here, we describe the native state, observable intermediate state, and unfolded state for ETR-3 RRM-3, which has canonical RRM fold. These observations can shed more light on unfolding events for RRM-containing proteins.     

Conformational forces affecting the folding pathways of dendrotoxins I and K from black mamba venom

The conformations of the major intermediates trapped during the folding of dendrotoxins I and K from venom of black mamba snakes, have been investigated by circular-dichroism spectroscopy. Local alterations to the native, folded conformations are observed in toxins I and K and in a protein of similar sequence, bovine pancreatic trypsin inhibitor. The inability of intermediates (30-51, 14-38) to complete refolding by forming directly the 5-55 disulphide bond is explained. The following observations on the role of secondary structure in the folding of the three proteins are of interest. 1. It is not necessary for the three proteins to acquire elements of secondary structure at the same stage of folding in order to attain similar three-dimensional conformations. 2. The stability of the final folded state is not directly correlated to an early appearance of secondary structure. 3. The degree of secondary structure already present in intermediates (30-51) seems to determine the pathway of refolding preferred by the corresponding protein.     

Thermodynamics and folding kinetics analysis of the SH3 domain form discrete molecular dynamics

We perform a detailed analysis of the thermodynamics and folding kinetics of the SH3 domain fold with discrete molecular dynamic simulations. We propose a protein model that reproduces some of the experimentally observed thermodynamic and folding kinetic properties of proteins. Specifically, we use our model to study the transition state ensemble of the SH3 fold family of proteins, a set of unstable conformations that fold to the protein native state with probability 1/2. We analyze the participation of each secondary structure element formed at the transition state ensemble. We also identify the folding nucleus of the SH3 fold and test extensively its importance for folding kinetics. We predict that a set of amino acid contacts between the RT-loop and the distal hairpin are the critical folding nucleus of the SH3 fold and propose a hypothesis that explains this result.     

Secondary-structure analysis of denatured proteins by vacuum-ultraviolet circular dichroism spectroscopy

To elucidate the structure of denatured proteins, we measured the vacuum-ultraviolet circular dichroism (VUVCD) spectra from 260 to 172 nm of three proteins (metmyoglobin, staphylococcal nuclease, and thioredoxin) in the native and the acid-, cold-, and heat-denatured states, using a synchrotron-radiation VUVCD spectrophotometer. The circular dichroism spectra of proteins fully unfolded by guanidine hydrochloride (GdnHCl) were also measured down to 197 nm for comparison. These denatured proteins exhibited characteristic VUVCD spectra that reflected a considerable amount of residual secondary structures. The contents of alpha-helices, beta-strands, turns, poly-L-proline type II (PPII), and unordered structures were estimated for each denatured state of the three proteins using the SELCON3 program with Protein Data Bank data and the VUVCD spectra of 31 reference proteins reported in our previous study. Based on these contents, the characteristics of the four types of denaturation were discussed for each protein. In all types of denaturation, a decrease in alpha-helices was accompanied by increases in beta-strands, PPII, and unordered structures. About 20% beta-strands were present even in the proteins fully unfolded by GdnHCl in which beta-sheets should be broken. From these results, we propose that denatured proteins constitute an ensemble of residual alpha-helices and beta-sheets, partly unfolded (or distorted) alpha-helices and beta-strands, PPII, and unordered structures.     

Molecular simulations of cotranslational protein folding: fragment stabilities, folding cooperativity, and trapping in the ribosome

Although molecular simulation methods have yielded valuable insights into mechanistic aspects of protein refolding in vitro, they have up to now not been used to model the folding of proteins as they are actually synthesized by the ribosome. To address this issue, we report here simulation studies of three model proteins: chymotrypsin inhibitor 2 (CI2), barnase, and Semliki forest virus protein (SFVP), and directly compare their folding during ribosome-mediated synthesis with their refolding from random, denatured conformations. To calibrate the methodology, simulations are first compared with in vitro data on the folding stabilities of N-terminal fragments of CI2 and barnase; the simulations reproduce the fact that both the stability and thermal folding cooperativity increase as fragments increase in length. Coupled simulations of synthesis and folding for the same two proteins are then described, showing that both fold essentially post-translationally, with mechanisms effectively identical to those for refolding. In both cases, confinement of the nascent polypeptide chain within the ribosome tunnel does not appear to promote significant formation of native structure during synthesis; there are however clear indications that the formation of structure within the nascent chain is sensitive to location within the ribosome tunnel, being subject to both gain and loss as the chain lengthens. Interestingly, simulations in which CI2 is artificially stabilized show a pronounced tendency to become trapped within the tunnel in partially folded conformations: non-cooperative folding, therefore, appears in the simulations to exert a detrimental effect on the rate at which fully folded conformations are formed. Finally, simulations of the two-domain protease module of SFVP, which experimentally folds cotranslationally, indicate that for multi-domain proteins, ribosome-mediated folding may follow different pathways from those taken during refolding. Taken together, these studies provide a first step toward developing more realistic methods for simulating protein folding as it occurs in vivo.     

Disorder-to-order conformational transitions in protein structure and its relationship to disease

Function in proteins largely depends on the acquisition of specific structures through folding at physiological time scales. Under both equilibrium and non-equilibrium states, proteins develop partially structured molecules that being intermediates in the process, usually resemble the structure of the fully folded protein. These intermediates, known as molten globules, present the faculty of adopting a large variety of conformations mainly supported by changes in their side chains. Taking into account that the mechanism to obtain a fully packed structure is considered more difficult energetically than forming partially “disordered” folding intermediates, evolution might have conferred upon an important number of proteins the capability to first partially fold and—depending on the presence of specific partner ligands—switch on disorder-to-order transitions to adopt a highly ordered well-folded state and reach the lowest energy conformation possible. Disorder in this context can represent segments of proteins or complete proteins that might exist in the native state. Moreover, because this type of disorder-to-order transition in proteins has been found to be reversible, it has been frequently associated with important signaling events in the cell. Due to the central role of this phenomenon in cell biology, protein misfolding and aberrant disorder-to-order transitions have been at present associated with an important number of diseases.     

Computer simulations of protein folding by targeted molecular dynamics

We have performed 128 folding and 45 unfolding molecular dynamics runs of chymotrypsin inhibitor 2 (CI2) with an implicit solvation model for a total simulation time of 0.4 microseconds. Folding requires that the three-dimensional structure of the native state is known. It was simulated at 300 K by supplementing the force field with a harmonic restraint which acts on the root-mean-square deviation and allows to decrease the distance to the target conformation. High temperature and/or the harmonic restraint were used to induce unfolding. Of the 62 folding simulations started from random conformations, 31 reached the native structure, while the success rate was 83% for the 66 trajectories which began from conformations unfolded by high-temperature dynamics. A funnel-like energy landscape is observed for unfolding at 475 K, while the unfolding runs at 300 K and 375 K as well as most of the folding trajectories have an almost flat energy landscape for conformations with less than about 50% of native contacts formed. The sequence of events, i.e., secondary and tertiary structure formation, is similar in all folding and unfolding simulations, despite the diversity of the pathways. Previous unfolding simulations of CI2 performed with different force fields showed a similar sequence of events. These results suggest that the topology of the native state plays an important role in the folding process.