Detection of an intermediate in the folding of the (beta alpha)8-barrel N-(5'-phosphoribosyl)anthranilate isomerase from Escherichia coli

We have used thermodynamic and kinetic techniques to monitor the guanidinium chloride induced (GdmCl-induced) denaturation of N-(5'-phosphoribosyl)anthranilate isomerase from Escherichia coli (ePRAI). Although CD-monitored equilibrium denaturation curves are consistent with cooperative unfolding of the protein centered at 1.45 M GdmCl, fluorescence readings drop by over 25% in the region preceding the CD-monitored transition, suggesting non-two-state behavior. Kinetics experiments measure a slow relaxation rate with negative fluorescence amplitude when protein is diluted from 0 to 0.5 M GdmCl, corroborating results from equilibrium conditions. Detection of several unfolding and refolding rates in final GdmCl concentrations from 0 to 5.0 M indicates the presence of at least one intermediate along unfolding and refolding pathways. GdmCl dependence of the relaxation rates can be explained most easily by a nonsequential mechanism for ePRAI unfolding, though a sequential mechanism cannot be ruled out. The data corroborate the fragment complementation studies of Eder and Kirschner [Eder, J., & Kischner, K. (1992) Biochemistry 31, 3617-3625], which are consistent with unfolding of the C-terminal portion of a yeast-derived PRAI in its folding intermediate. In ePRAI, such partial unfolding would expose W391 to quenching by solvent molecules; W356, ePRAI's other tryptophan, is buried in the hydrophobic core and is unlikely to be affected by local changes in structure. A C-terminally unfolded folding intermediate has been demonstrated in the folding of tryptophan synthase (alpha-subunit), a related beta alpha-barrel enzyme.(ABSTRACT TRUNCATED AT 250 WORDS)     

Thermodynamic characterization of the conformational stability of the homodimeric protein, pea lectin

The conformational stability of the homodimeric pea lectin was determined by both isothermal urea-induced and thermal denaturation in the absence and presence of urea. The denaturation profiles were analyzed to obtain the thermodynamic parameters associated with the unfolding of the protein. The data not only conform to the simple A2 if 2U model of unfolding but also are well described by the linear extrapolation model for the nature of denaturant-protein interactions. In addition, both the conformational stability (DeltaGs) and the DeltaCp for the protein unfolding is quite high, at about 18.79 kcal/mol and 5.32 kcal/(mol K), respectively, which may be a reflection of the relatively larger size of the dimeric molecule (Mr 49 000) and, perhaps, a consequent larger buried hydrophobic core in the folded protein. The simple two-state (A2 if 2U) nature of the unfolding process, with the absence of any monomeric intermediate, suggests that the quaternary interactions alone may contribute significantly to the conformational stability of the oligomer-a point that may be general to many oligomeric proteins.     

Thermodynamic characterization of the coupled folding and association of heterodimeric coiled coils (leucine zippers)

Folding thermodynamics of nine heterodimeric, parallel coiled coils were studied by isothermal titration calorimetry (ITC) and thermal unfolding circular dichroism measurements. The heterodimers were composed of an acidic and a basic 30-residue peptide, which when in isolation were monomeric and essentially unstructured. The reaction followed a two-state mechanism indicating that folding and association were coupled. delta Hfold, delta Sfold and delta Cp normalized per mol of residue were of the same magnitude as for monomeric globular proteins, hence the energetics of folding and association of the heterodimeric coiled coils was balanced similarly to the folding of a single polypeptide chain. Cavity creating Leu/Ala substitutions revealed strong and position-dependent energetic coupling between leucine residues in the hydrophobic core of the coiled coil. delta Gunfold (equivalent to -delta Gfold in the two-state reaction) was determined from thermal unfolding. Global stability curves were calculated according to the Gibbs-Helmholtz equation and using the combined free energy data from ITC and thermal unfolding. Maximum stabilities were between 15 and 37 degrees C and cold denaturation could be demonstrated by direct calorimetry. The stability curves were based on free energies of folding measured between 10 and 85 degrees C and under identical solvent conditions. This represents a novel experimental approach which circumvents the use of varying solvent conditions as is typically required to measure protein stability curves. Discrepancies were noticed between van't Hoff enthalpies deduced from thermal unfolding and measured by direct calorimetry. The discrepancies are thought to be due to residual ordered structure in the denatured single chains around room temperature but not near the transition midpoint temperature Tm. This demonstrates that over an extended temperature range the assumption of a common denatured state implicit in the van't Hoff analysis may not always be valid.     

Fast and one-step folding of closely and distantly related homologous proteins of a four-helix bundle family

Bovine acyl-coenzyme A binding protein is a four-helix bundle protein belonging to a group of homologous eukaryote proteins that binds medium and long-chain acyl-coenzyme A esters with a very high affinity. The three-dimensional structure of both the free and the ligated protein together with the folding kinetics have been described in detail for the bovine protein and with four new sequences reported here, a total of 16 closely related sequences ranging from yeasts and plants to human are known. The kinetics of folding and unfolding in different concentrations of guanidine hydrochloride together with equilibrium unfolding have been measured for bovine, rat and yeast acyl-coenzyme A binding protein. The bovine and rat sequences are closely related whereas the yeast is more distantly related to these. In addition to the three natural variants, kinetics of a bovine mutant protein, Tyr31 --> Asn, have been studied. Both the folding and unfolding rates in water of the yeast protein are 15 times faster than those of bovine. The folding rates in water of the two mammalian forms, rat and bovine, are similar, though still significantly different. A faster unfolding rate both for rat and the bovine mutant protein results from a lower stability of the native states of these. These hydrophobic regions, mini cores, have been identified in the three-dimensional structure of the bovine protein and found to be formed primarily by residues that have been conserved throughout the entire eukaryote evolution from yeasts to both plants and mammals as seen in the sample of 16 sequences. The conserved residues are found to stabilize helix-helix interactions and serve specific functional purposes for ligand binding. The fast one-step folding mechanism of ACBP has been shown to be a feature that seems to be maintained throughout evolution despite numerous differences in sequence and even dramatic differences in folding kinetics and protein stability. The protein study raises the question to what extent does the conserved hydrophobic residues provide a scaffold for an efficient one-step folding mechanism.     

Simulating the minimum core for hydrophobic collapse in globular proteins

To investigate the nature of hydrophobic collapse considered to be the driving force in protein folding, we have simulated aqueous solutions of two model hydrophobic solutes, methane and isobutylene. Using a novel methodology for determining contacts, we can precisely follow hydrophobic aggregation as it proceeds through three stages: dispersed, transition, and collapsed. Theoretical modeling of the cluster formation observed by simulation indicates that this aggregation is cooperative and that the simulations favor the formation of a single cluster midway through the transition stage. This defines a minimum solute hydrophobic core volume. We compare this with protein hydrophobic core volumes determined from solved crystal structures. Our analysis shows that the solute core volume roughly estimates the minimum core size required for independent hydrophobic stabilization of a protein and defines a limiting concentration of nonpolar residues that can cause hydrophobic collapse. These results suggest that the physical forces driving aggregation of hydrophobic molecules in water is indeed responsible for protein folding.     

p53 protein accumulation and response to adjuvant chemotherapy in premenopausal women with node-negative early breast cancer

Although beta-sheets represent a sizable fraction of the secondary structure found in proteins, the forces guiding the formation of beta-sheets are still not well understood. Here we examine the folding of a small, all beta-sheet protein, the E. coli major cold shock protein CspA, using both equilibrium and kinetic methods. The equilibrium denaturation of CspA is reversible and displays a single transition between folded and unfolded states. The kinetic traces of the unfolding and refolding of CspA studied by stopped-flow fluorescence spectroscopy are monoexponential and thus also consistent with a two-state model. In the absence of denaturant, CspA refolds very fast with a time constant of 5 ms. The unfolding of CspA is also rapid, and at urea concentrations above the denaturation midpoint, the rate of unfolding is largely independent of urea concentration. This suggests that the transition state ensemble more closely resembles the native state in terms of solvent accessibility than the denatured state. Based on the model of a compact transition state and on an unusual structural feature of CspA, a solvent-exposed cluster of aromatic side chains, we propose a novel folding mechanism for CspA. We have also investigated the possible complications that may arise from attaching polyhistidine affinity tags to the carboxy and amino termini of CspA.     

A step toward understanding the folding mechanism of bovine adrenodoxin

The iron-sulfur clusters of iron-sulfur proteins are not only essential for the structure and function but they also seem to play an important role in the folding process of these proteins. So far, no data on reversible unfolding/refolding of iron-sulfur proteins under aerobic conditions have been reported. We found appropriate conditions, which might also be applicable for other iron-sulfur proteins, for reversible unfolding/refolding of bovine adrenodoxin (Adx) that prevent cluster decomposition during the unfolding process. The unfolding/refolding studies have been performed under aerobic conditions using fluorescence measurements (with mutant Y82W of Adx, providing a sensitive internal probe), absorption, and circular dichroism (CD) spectroscopy as well as activity measurements. Without protecting reagent, adrenodoxin becomes an apoprotein upon denaturation which is an irreversible process with respect to cluster rebinding. However, reversibility of unfolding/refolding can be observed after protein denaturation in the presence of dithiothreitol (DTT). Upon removal of the denaturant, we regained 65, 63, and 64% refolding from CD, fluorescence, and activity measurements, respectively. In the case of thermal denaturation, the percentage of refolding is about 60% according to CD measurements. DTT appears to stabilize the [2Fe-2S] cluster and prevents its decomposition during aerobic unfolding, providing thereby the means of correct refolding of the protein.     

Equilibrium unfolding of proteins monitored by electrospray ionization mass spectrometry: distinguishing two-state from multi-state transitions

The acetic acid-induced unfolding of cytochrome c (cyt c) and apomyoglobin (aMb) are studied under equilibrium conditions by electrospray ionization (ESI) mass spectrometry (MS). The folding states of the proteins in solution are monitored by the charge state distributions that they produce during ESI. A tightly folded protein shows lower charge states than the same protein in an unfolded conformation. The ESI-MS data presented in this study show that during the denaturation of cyt c, only two distinct charge state distributions are observed. These can be attributed to the native and to the acid-unfolded conformation, respectively. In the transition region where the folded and the unfolded conformation are both present in solution, these two distributions are observed simultaneously, thus giving rise to a bimodal ESI mass spectrum. These data reflect a highly cooperative (two state) folding behavior. In contrast, the acid-induced unfolding of aMb is accompanied by gradual shifts in the maxima of the observed charge state distribution. This indicates a non-cooperative unfolding behavior involving multiple protein conformations. The observations made here suggest that ESI-MS might be a general method for assessing the cooperativity of protein unfolding transitions. This study also addresses the issue of 'secondary' solvent effects for ESI-MS studies on the acid-induced unfolding of proteins. These effects influence the ESI charge state distribution without being related to conformational changes of the protein in solution and could potentially complicate the interpretation of ESI mass spectra. Data obtained for bovine pancreatic trypsin inhibitor and ubiquitin indicate that secondary solvent effects influence the observed charge state distributions only to a very minor extent between pH 8.5 and 2.5.     

Discrete molecular dynamics studies of the folding of a protein-like model

BACKGROUND: Many attempts have been made to resolve in time the folding of model proteins in computer simulations. Different computational approaches have emerged. Some of these approaches suffer from insensitivity to the geometrical properties of the proteins (lattice models), whereas others are computationally heavy (traditional molecular dynamics). RESULTS: We used the recently proposed approach of Zhou and Karplus to study the folding of a protein model based on the discrete time molecular dynamics algorithm. We show that this algorithm resolves with respect to time the folding <--> unfolding transition. In addition, we demonstrate the ability to study the core of the model protein. CONCLUSIONS: The algorithm along with the model of interresidue interactions can serve as a tool for studying the thermodynamics and kinetics of protein models.     

The single helix in protein L is largely disrupted at the rate-limiting step in folding

To investigate the role of helix formation in the folding of protein L, a 62 residue alpha/beta protein, we studied the consequences of both single and multiple mutations in the helix on the kinetics of folding. A triple mutant with 11 additional carbon atoms in core residues in the amino-terminal portion of the helix folded substantially faster than wild type, suggesting that hydrophobic association with residues elsewhere in the protein occurs at the rate-limiting step in folding. However, helix-destabilizing mutations had little effect on the rate of folding; in particular, a triple glycine substitution on the solvent-exposed side of the helix increased the unfolding rate 56-fold while reducing the folding rate less than threefold. Thus, in contrast to the predictions of models of folding involving the coalescence of well-formed secondary structure elements, the single helix in protein L appears to be largely disrupted at the rate-limiting step in folding and unfolding.     

Urea and thermal equilibrium denaturation studies on the dimerization domain of Escherichia coli Trp repressor

The urea-induced equilibrium unfolding of the Escherichia coli Trp repressor (TR) is a two-state process, involving the native dimeric and unfolded monomeric species. Kinetic studies, however, reveal the presence of transient intermediates that appear only during the folding of the 107-residue protein [Gittelman, M. G., & Matthews, C. R. (1990) Biochemistry 29, 7011-7020]. In order to gain insight into the complex kinetic folding mechanism, the sequence of TR was reduced to the amino-terminal 66 residues, corresponding to the dimerization domain. Two polypeptides, 2-66 and NHis-7-66, were shown to be dimeric at 25 degrees C by size exclusion chromatography and to retain native-like spectroscopic features as evidenced by near- and far-UV circular dichroism and fluorescence spectroscopy. The equilibrium properties of the urea-induced folding of these core fragments were examined by intrinsic tryptophan fluorescence and circular dichroism and found to be well described by a two-state model. At 25 degrees C, the stabilities of both fragments are 14 kcal mol(-1), as compared to the 24 kcal mol(-1) observed for full-length TR. In contrast, the thermal denaturation of [2-66]2 and full-length TR are three-state processes; the midpoint of the transition monitored by absorbance at 292 nm precedes that monitored by circular dichroism at 222 nm. Global analysis of the thermal data as a function of monomer concentration suggests that both the full-length and [2-66]2 TR variants unfold via a dimeric intermediate. Taken together, these results demonstrate that the [2-66]2 fragment constitutes a well-structured, independently folding subdomain of TR that may be useful in elucidating the properties of the transient intermediates observed in the folding of the full-length protein. The dimeric intermediate observed in the thermal denaturation of [2-66]2 suggests that it may be possible to further reduce the core sequence while maintaining the ability to dimerize.     

The burst-phase intermediate in the refolding of beta-lactoglobulin studied by stopped-flow circular dichroism and absorption spectroscopy

The kinetics of the guanidine hydrochloride-induced unfolding and refolding of bovine beta-lactoglobulin, a predominantly beta-sheet protein in the native state, have been studied by stopped-flow circular dichroism and absorption measurements at pH 3.2 and 4.5 degrees C. The refolding reaction was a complex process composed of different kinetic phases, while the unfolding was a single-phase reaction. Most notably, a burst-phase intermediate of refolding, which was formed during the dead time of stopped-flow measurements (approximately 18 ms), showed more intense ellipticity signals in the peptide region below 240 nm than the native state, yielding overshoot behavior in the refolding curves. We have investigated the spectral properties and structural stability of the burst-phase intermediate and also the structural properties in the unfolded state in 4.0 M guanidine hydrochloride of the protein and its disulfide-cleaved derivative. The main conclusions are: (1) the more intense ellipticity of the intermediate in the peptide region arises from formation of non-native alpha-helical structure in the intermediate, apparently suggesting that the folding of beta-lactoglobulin is not represented by a simple sequential mechanism. (2) The burst-phase intermediate has, however, a number of properties in common with the folding intermediates or with the molten globule states of other globular proteins whose folding reactions are known to be represented by the sequential model. These properties include: the presence of the secondary structure without the specific tertiary structure; formation of a hydrophobic core; broad unfolding transition of the intermediate; and rapidity of formation of the intermediate. The burst-phase intermediate of beta-lactoglobulin is thus classified as the same species as the molten globule state. (3) The circular dichroism spectra of beta-lactoglobulin and its disulfide-cleaved derivative in 4.0 M guanidine hydrochloride suggests the presence of the residual beta-structure in the unfolded state and the stabilization of the beta-structure by disulfide bonds. Thus; if this residual beta-structure is part of the native beta-structure and forms a folding initiation site, the folding reaction of beta-lactoglobulin may not necessarily be inconsistent with the sequential model. The non-native alpha-helices in the burst-phase intermediate may be formed in an immature part of the protein molecule because of the local alpha-helical propensity in this part.     

Cortical interneurons upregulate neurotrophins in vivo in response to targeted apoptotic degeneration of neighboring pyramidal neurons

The pressure-induced unfolding of wild-type staphylococcal nuclease (Snase WT) was studied using synchrotron X-ray small-angle scattering (SAXS) and Fourier-transform infrared (FT-IR) spectroscopy, which monitor changes in the tertiary and secondary structural properties of the protein upon pressurization. The experimental results reveal that application of high-pressure up to 3 kbar leads to an approximate twofold increase of the radius of gyration Rg of the native protein (Rg approximately 17 A) and a large broadening of the pair-distance-distribution function, indicating a transition from a globular to an ellipsoidal or extended chain structure. Analysis of the FT-IR amide I' spectral components reveals that the pressure-induced denaturation process sets in at 1.5 kbar at 25 degrees C and is accompanied by an increase in disordered and turn structures while the content of beta-sheets and alpha-helices drastically decreases. The pressure-induced denatured state above 3 kbar retains nonetheless some degree of beta-like secondary structure and the molecule cannot be described as a fully extended random coil. Temperature-induced denaturation involves a further unfolding of the protein molecule which is indicated by a larger Rg value and significantly lower fractional intensities of IR-bands associated with secondary-structure elements. In addition, we have carried out pressure-jump kinetics studies of the secondary-structural evolution and the degree of compactness in the folding/unfolding reactions of Snase. The effect of pressure on the kinetics arises from a larger positive activation volume for folding than for unfolding, and leads to a significant slowing down of the folding rate with increasing pressure. Moreover, the system becomes two-state under pressure. These properties make it ideal for probing multiple order parameters in order to compare the kinetics of changes in secondary structure by pressure-jump FT-IR and chain collapse by pressure-jump SAXS. After a pressure jump from 1 bar to 2.4 kbar at 20 degrees C, the radius of gyration increases in a first-order manner from 17 A to 22.4 A over a timescale of approximately 30 minutes. The increase in Rg value is caused by the formation of an extended (ellipsoidal) structure as indicated by the corresponding pair-distance-distribution function. Pressure-jump FT-IR studies reveal that the reversible first order changes in beta-sheet, alpha-helical and random structure occur on the same slow timescale as that observed for the scattering curves and for fluorescence. These studies indicate that the changes in secondary structure and chain compactness in the folding/unfolding reactions of Snase are probably dependent upon the same rate-limiting step as changes in tertiary structure.     

Analysing functional connectivity in brain slices by a combination of infrared video microscopy, flash photolysis of caged compounds and scanning methods

The equilibrium unfolding and the kinetics of unfolding and refolding of equine lysozyme, a Ca2+-binding protein, were studied by means of circular dichroism spectra in the far and near-ultraviolet regions. The transition curves of the guanidine hydrochloride-induced unfolding measured at 230 nm and 292.5 nm, and for the apo and holo forms of the protein have shown that the unfolding is well represented by a three-state mechanism in which the molten globule state is populated as a stable intermediate. The molten globule state of this protein is more stable and more native-like than that of alpha-lactalbumin, a homologous protein of equine lysozyme. The kinetic unfolding and refolding of the protein were induced by concentration jumps of the denaturant and measured by stopped-flow circular dichroism. The observed unfolding and refolding curves both agreed well with a single-exponential function. However, in the kinetic refolding reactions below 3 M guanidine hydrochloride, a burst-phase change in the circular dichroism was present, and the burst-phase intermediate in the kinetic refolding is shown to be identical with the molten globule state observed in the equilibrium unfolding. Under a strongly native condition, virtually all the molecules of equine lysozyme transform the structure from the unfolded state into the molten globule, and the subsequent refolding takes place from the molten globule state. The transition state of folding, which may exist between the molten globule and the native states, was characterized by investigating the guanidine hydrochloride concentration-dependence of the rate constants of refolding and unfolding. More than 80% of the hydrophobic surface of the protein is buried in the transition state, so that it is much closer to the native state than to the molten globule in which only 36% of the surface is buried in the interior of the molecule. It is concluded that all the present results are best explained by a sequential model of protein folding, in which the molten globule state is an obligatory folding intermediate on the pathway of folding.     

Equilibrium unfolding studies of barstar: evidence for an alternative conformation which resembles a molten globule

The folding of the small protein barstar, which is the intracellular inhibitor to barnase in Bacillus amyloliquefaciens, has been studied by equilibrium unfolding methods. Barstar is shown to exist in two conformations: the A form, which exists at pH values lower than 4, and the N state, which exists at pH values above 5. The transition between the A form and the N state is completely reversible. UV absorbance spectroscopy, fluorescence spectroscopy, and circular dichroism spectroscopy were used to study the two conformations. The mean residue ellipticity measured at 220 nm of the A form is 60% that of the N state, and the A form has some of the properties expected for a molten globule conformation. Fluorescence energy transfer experiments using 1-anilino-8-naphthalenesulfonate indicate that at least one of the three tryptophan residues in the A form is accessible to water. Surprisingly, high concentrations of denaturant are required to unfold the A form. For denaturation by guanidine hydrochloride, the midpoint of the cooperative unfolding transition measured by circular dichroism for the A form at pH 3 is 3.7 +/- 0.1 M, which is significantly higher than the value of 2.0 +/- 0.1 M observed for the N state at pH 7. The unfolding of the A form by guanidine hydrochloride or urea is complex and cannot be satisfactorily fit to a two-state (A<==>U) model for unfolding. Fluorescence-monitored tertiary structure melts before circular dichroism-monitored secondary structure, and an equilibrium unfolding intermediate must be present on the unfolding pathway of A.     

Characterization of the free energy spectrum of peptostreptococcal protein L

BACKGROUND: Native state hydrogen/deuterium exchange studies on cytochrome c and RNase H revealed the presence of excited states with partially formed native structure. We set out to determine whether such excited states are populated for a very small and simple protein, the IgG-binding domain of peptostreptococcal protein L. RESULTS: Hydrogen/deuterium exchange data on protein L in 0-1.2 M guanidine fit well to a simple model in which the only contributions to exchange are denaturant-independent local fluctuations and global unfolding. A substantial discrepancy emerged between unfolding free energy estimates from hydrogen/deuterium exchange and linear extrapolation of earlier guanidine denaturation experiments. A better determined estimate of the free energy of unfolding obtained by global analysis of a series of thermal denaturation experiments in the presence of 0-3 M guanidine was in good agreement with the estimate from hydrogen/deuterium exchange. CONCLUSIONS: For protein L under native conditions, there do not appear to be partially folded states with free energies intermediate between that of the folded and unfolded states. The linear extrapolation method significantly underestimates the free energy of folding of protein L due to deviations from linearity in the dependence of the free energy on the denaturant concentration.     

Titration properties and thermodynamics of the transition state for folding: comparison of two-state and multi-state folding pathways

CI2 folds and unfolds as a single cooperative unit by simple two-state kinetics, which enables the properties of the transition state to be measured from both the forward and backward rate constants. We have examined how the free energy of the transition state for the folding of chymotrypsin inhibitor 2 (CI2) changes with pH and temperature. In addition to the standard thermodynamic quantities, we have measured the overall acid-titration properties of the transition state and its heat capacity relative to both the denatured and native states. We were able to determine the latter by a method analogous to a well-established procedure for measuring the change in heat capacity for equilibrium unfolding: the enthalpy of activation of unfolding at different values of acid pH were plotted against the average temperature of each determination. Our results show that the transition state of CI2 has lost most of the electrostatic and van der Waals' interactions that are found in the native state, but it remains compact and this prevents water molecules from entering some parts of the hydrophobic core. The properties of the transition state of CI2 are then compared with the major folding transition state of the larger protein barnase, which folds by a multi-state mechanism, with the accumulation of a partly structured intermediate (Dphys or I). CI2 folds from a largely unstructured denatured state under physiological conditions via a transition state which is compact but relatively uniformly unstructured, with tertiary and secondary structure being formed in parallel. We term this an expanded pathway. Conversely, barnase folds from a largely structured denatured state in which elements of structure are well formed through a transition state that has islands of folded elements of structure. We term this a compact pathway. These two pathways may correspond to the two extreme ends of a continuous spectrum of protein folding mechanisms. Although the properties of the two transition states are very different, the activation barrier for folding (Dphys-->++) is very similar for both proteins.     

Seasonal regulation of prolactin secretion in hypophyseal stalk transected beef calves

Conformational transitions of holo-alpha-lactalbumin in a hydro-ethanolic cosolvent system was studied by spectrofluorescence, CD in near- and far-uv regions, and high-sensitivity differential scanning calorimetry. Experimental results allow us to propose that in isothermal conditions alpha-lactalbumin undergoes a number of conformational transitions with increasing ethanol concentration: N<=>I<=>D<=>H. The existence of I-state was deduced from spectrofluorometric and near-uv CD data. In this state the aromatic chromophores of the amino acid side chains are more accessible to the solvent displaying higher local mobility. The H-state was detected from far-uv CD spectra as a state corresponding to the content of alpha-helices higher than originally found in native protein. However, calorimetric measurements provide data revealing only the two-state mechanism of alpha-lactalbumin unfolding in both water and in aqueous ethanol solutions. This indicates that the energy levels of N- and I-states as well as of D- and H-states are similar. Thermodynamics of the unfolding of alpha-lactalbumin in hydroethanolic solutions was analyzed with the help of the linear model of solvent denaturation. Unfolding increments of enthalpy, entropy, and Gibbs energy of transfer of the protein from a reference aqueous solution to hydro-ethanolic solutions of different concentrations were determined from the calorimetric data. They are linear functions of molar ethanol fraction. The slope of the unfolding increment of Gibbs energy of transfer was calculated from data on transfer of amino acid residues taking into account the average solvent accessibility of amino acid residues in the native structure of small globular proteins, using the additive group contribution method.     

Fragment reconstitution of a small protein: folding energetics of the reconstituted immunoglobulin binding domain B1 of streptococcal protein G

To elucidate early stages in protein folding, we have adopted a fragment reconstitution method for small proteins. This approach is expected to provide nuclei for protein folding and to allow us to investigate folding mechanisms. In previous work [Kobayashi, N., et al. (1995) FEBS Lett. 366, 99-103.] we demonstrated the association of two complementary fragments, derived from the immunoglobulin G-binding domain B1 of streptococcal Protein G, and showed the structural similarity between the reconstituted domain and the uncleaved wild-type domain. In this work we have further characterized the reconstituted domain as well as the uncleaved domain thermodynamically by means of differential scanning calorimetry (DSC) and circular dichroism (CD) measurements. Although composed of short peptide fragments not linked by covalent bonds, the reconstituted domain showed a typical folding/unfolding curve in both DSC and CD melting measurements and behaved like a globular protein. The domain was not very stable, and the small value of the Gibbs free energy corresponded to the class of the weakest protein-protein binding systems. The denaturation temperature of 0. 78 mM solution was 313 K at pH 5.9 as measured by DSC, which was more than 40 degrees lower than the uncleaved domain. This apparent instability was primarily caused by entropic disadvantage attributed to a bimolecular reaction. The temperature dependence of the enthalpy change from the folded to the unfolded state was almost identical for the reconstituted domain and the uncleaved one. This indicates that most of the noncovalent intramolecular interactions stabilizing the native structure, such as hydrogen bonding and hydrophobic interactions, are regenerated in the reconstituted domain. By comparing the equilibrium constants of the reconstituted and uncleaved domains, we determined the effective concentration to be approximately 6 M at 298 K. Structure-based estimation of the thermodynamic properties from the values of accessible surface areas showed that approximately 35% of the total heat capacity change and approximately 25% of the total enthalpy change can be attributed to the interchain interaction at 298 K. Furthermore, the folding/unfolding equilibrium of beta-hairpin structure of the fragment 41-56 alone was also characterized. These analyses allow us to envision the microdomain folding mechanism of the Protein G B1 domain, in which segment 41-56 first forms a stable beta-hairpin structure and then collides with segment 1-40, followed by spontaneous folding of the whole molecule.     

Situation determinants of heroin consumption in opiate-dependent subjects: a psychometric approach

BACKGROUND: Chymotrypsin inhibitor 2 (CI2) is a member of the class of fast-folding small proteins, which is very suitable for testing theories of folding. CI2 folds around a diffuse extended nucleus consisting of the single alpha helix and a set of hydrophobic residues. In particular, Ala16 has been predicted and independently found to interact with Leu49 and Ile57, hydrophobic residues that are highly conserved among homologues. We have characterised in detail the interactions between these residues in the folding nucleus of the protein by using double-mutant cycles. RESULTS: Surprisingly, we find that there is some destabilising strain in the transition state for folding of the wild-type protein between Ala16 and Ile57. Further, we find that the strain is larger in the native state of the protein. This is shown directly in the unfolding kinetics, which clearly show a release of strain. The net result of this is that the presence of both residues speeds up folding. Ala16 and Leu49 interact favourably in the transition state, but have no net interaction energy in the native state. CONCLUSIONS: Part of the folding nucleus of the protein fits together more snugly in the transition state than it does in the native state. Interactions between some of the closely packed residues in the folding nucleus of CI2 may perhaps be optimised for the rate of folding and not for stability.