Differential inhibition of lysophosphatidate signaling by volatile anesthetics

cAMP receptor protein (CRP) is involved in regulation of expression of several genes in Escherichia coli. The protein is a homodimer and each monomer is folded into two distinct structural domains. The mechanism of the biological activity of the protein may involve the interaction between the subunits and domains. In order to determine the interaction between the subunits or domains of CRP, we have studied the reversible denaturation of the protein by guanidine hydrochloride. The unfolding and refolding kinetics of CRP was monitored using stopped-flow fluorescence spectroscopy at 20 degrees C and pH 7.9. The results of CRP denaturation indicate that the transition can be described by a three-state model: (CRP native)2<=> 2 (CRP native)<=>2 (CRP denatured). The faster process, characterized by the relaxation time tau 2 = 80 +/- 3 ms, corresponds to the dissociation of CRP dimer into monomers. The slower process has the relaxation time tau t = 1.9 +/- 0.1 s and corresponds to the cooperative unfolding of CRP monomer. The free energy change in the absence of denaturant upon CRP dissociation is delta G dis degrees = 46.9 +/- 2.5 kJ/mol and for monomer unfolding delta G unf degrees = 30.9 +/- 1.3 kJ/mol. The thermal unfolding of CRP was studied by circular dichroism and fluorescence spectroscopy at various guanidine hydrochloride concentrations. It has been found that the native protein is maximally stable at about 21 +/- 0.3 degrees C and is denatured upon heating and cooling from this temperature. The apparent free energy change for CRP unfolding at 21 degrees C is equal to 30.5 +/- 0.4 kJ/mol and the apparent specific heat change is equal to delta Cp, app = 10.7 +/- 0.7 kJ mol-1 K-1. The predicted values of cold denaturation midpoint is equal to tau G = -18.8 +/- 1.5 degrees C and for high-temperature transition tau G = 63.1 +/- 1.5 degrees C. The predicted midpoint of high-temperature unfolding transition is about the same as determined experimentally.     

Chemical and thermal stability of ferulic acid esterase-III from Aspergillus niger

The stability of ferulic acid esterase III (FAE-III) from Aspergillus niger was examined using chemical and thermal denaturation. Thermal denaturation was irreversible and the loss of activity was dependent on pH. At 60 degrees C and pH 6.0, the rate constant of unfolding was 0.76 10(-3)/s, and the change in free energy of irreversible inactivation, deltaG*, was 101.9 kJ/mol. Sinapic acid, a product of the reaction of methyl sinapate with FAE-III, reduced the rate of unfolding (0.66 10(-3)/s at 0.1 mM sinapic acid). Chemical denaturation was performed using guanidine hydrochloride. FAE-III was very sensitive to this denaturant, and the midpoint of unfolding was 1.38 M guanidine hydrochloride at 30 degrees C, pH 6.0. The stability of FAE-III is compared to other enzymes.     

Conformation and unfolding thermodynamics of epidermal growth factor and derivatives

Mouse submaxillary epidermal growth factor (EGF) is a 53-residue single chain peptide hormone of known amino acid sequence which contains three disulfides, five tyrosines, and two tryptophans. Circular dichroic (CD) spectra have been obtained and resolved for EGF, several well-characterized chemical and enzymic derivatives, and related low molecular weight model compounds. Assignments have been made to most of the resolved bands; these include the peptide, aromatic, and disulfide chromophores. From a comparison of the rotational strength of the 213-nm resolved CD band in native EGF with that of standard proteins, EGF is estimated to contain about 22% beta structure and no alpha helicity. A derivative of EGF lacking the five carboxyl-terminal residues (prepared by limited trypsin digestion) and the cyanogen bromide derivative, in which there is a single main-chain cleavage at residue 21, have spectra properties indicative of approximately 10 and 12% beta structure, respectively. The near-ultraviolet CD spectra of the derivatives are similar to, albeit not identical with, that of EGF. The rotational strengths characteristic of the side-chain chromophores in EGF and these derivatives are several-fold higher than the corresponding values in low molecular weight model compounds. Thus, it appears that EGF and these modified forms contain a stable (and similar) tertiary structure. In contrast, the S-aminoethylated derivative of EGF exhibits a drastically altered CD spectrum relative to EGF indicating a different conformation(s). Equilibrium studies on the guanidinium hydrochloride (GdmCl) mediated reversible unfolding of EGF showed that the transition midpoint is quite high (i.e., 6.89 M GdmCl at 25.0 degrees C), thus, indicating considerable stability. From these data a rough estimate of 16 kcal/mol can be made for the unfolding free energy (delta G degrees) of EGF in the absence of denaturant. Interestingly, EGF exhibits greater stability characteristics than several proteins two to four times its size. The cyanogen bromide derivative of EGF exhibited greatly reduced stability characteristics, e.g., the transition midpoint occurred at 4.19 M GdmCl (25.0 degrees C) and delta G degrees was estimated to be approximately 4 kcal/mol. Thus, a single main-chain cleavage reduced the stability of EGF by about 70%. Thermal transitions of EGF and the cyanogen bromide derivative in the presence of concentrated GdmCl are characterized by a relatively high enthalpy of about 25 kcal/mol at 40 degrees C and a low (probably zero) heat capacity. From these thermodynamic parameters one can calculate that the large reduction in delta G degrees due to scission of the single peptide bond between residues 21 and 22 can be attributed almost completely to a change in entropy; e.g., at 40 degrees C the apparent entropy of unfolding of EGF is 20.4 cal mol-1 deg-1 while that of the cyanogen bromide derivative is 66.4 cal mol-1 deg-1.     

Cooperative folding of a protein mini domain: the peripheral subunit-binding domain of the pyruvate dehydrogenase multienzyme complex

The peripheral subunit-binding domain from the dihydrolipoamide acetyltransferase (E2) component of the pyruvate dehydrogenase multienzyme complex from Bacillus stearothermophilus is stably folded, despite its short sequence of only 43 amino acid residues. A 41 residue peptide derived from this domain, psbd41, undergoes a cooperative thermal unfolding transition with a tm of 54 degrees C. This three-helix protein is monomeric as judged by ultracentrifugation and concentration-dependent CD measurements. Peptides corresponding to the individual helices are largely unstructured both alone and in combination, indicating that the unusual stability of this protein does not arise solely from unusually stable alpha-helices. Chemical denaturation by guanidine hydrochloride is also cooperative with a delta GH2O of 3.1 kcal mol-1 at pH 8.0 and 25 degrees C. The chemical denaturation is broad with an m-value of 760 cal mol-1 M-1. psbd41 contains a buried aspartate residue at position 34 that may provide stability and specificity to the fold. A mutant peptide, psbd41Asn was synthesized in which the buried aspartate residue was mutated to asparagine. This peptide still folds cooperatively and it is monomeric, but is much less thermostable than the wild-type with a tm of only 31 degrees C. Chemical denaturations at 4 degrees C give an m-value of 740 cal mol-1 M-1, similar to the wild-type, but the stability delta GH2O is only 1.4 kcal mol-1. Both the wild-type and the mutant unfold at extremes of pH, but at 4 degrees C psbd41Asn is folded over a narrower pH range than the wild-type. Although the mutant unfolds cooperatively by thermal and by chemical denaturation, its NMR spectrum is significantly broader than that of the wild-type and it binds ANS. These results show that Asp34 is vital for the stability and specificity of this structure, the second smallest natural sequence known to fold in the absence of disulfide bonds or metal or ligand-binding sites.     

Isotopic survival criteria of transfused polymorphonuclear cells

The enthalpies of interaction of urea with five globular proteins, ribonuclease A, trypsin, beta-lacto-globulin, ovalbumin and bovine serum albumin have been measured in aqueous solution at pH 7.0, I=0.005 M and 25 degrees C over a range of urea molality m from 0-15 mmol g-1 (where a 1 molal solution contains 1 mmol g-1). For all the proteins the interaction is exothermic, and there is an appreciable heat evolution at low urea concentrations, m less than 5 mmol g-1, which increases sharply at higher urea concentrations when the proteins undergo unfolding. If account is taken of the endothermic enthalpies of unfolding of the native proteins, the enthalpies of interactions of urea per unit mass denatured protein lie in the range -45 to -75 J g-1, corresponding to an average binding enthalpy of -23 kJ mol-1 bound urea.     

Protein denaturation: a small-angle X-ray scattering study of the ensemble of unfolded states of cytochrome c

Solution X-ray scattering was used to study the equilibrium unfolding of cytochrome c as a function of guanidine hydrochloride concentration at neutral pH. The radius of gyration (Rg) shows a cooperative transition with increasing denaturant with a similar Cm to that observed with circular dichroism. However, the lack of an isoscattering point in the X-ray scattering patterns suggests the equilibrium unfolding is not simply a two-state process. Singular value decomposition (SVD) analysis was applied to the scattering patterns to determine the number of distinct scattering species. SVD analysis reveals the existence of three components, suggesting that at least three equilibrium states of the protein exist. A model was employed to determine the thermodynamic parameters and the scattering profiles of the three equilibrium states. These scattering profiles show that one state is native (N). The other two states (U1, U2) are unfolded, with U2 being fully unfolded and U1 having some residual structure. Using the thermodynamic parameters to calculate fractional populations, U1 is maximally populated at intermediate denaturant concentrations while U2 is maximally populated at high denaturant concentrations. It is likely that there is a multiplicity of denatured states with U1 and U2 representing an average of the denatured states populated at intermediate and high denaturant concentrations, respectively.     

Global analysis of the thermal and chemical denaturation of the N-terminal domain of the ribosomal protein L9 in H2O and D2O. Determination of the thermodynamic parameters, deltaH(o), deltaS(o), and deltaC(o)p and evaluation of solvent isotope effects

The stability of the N-terminal domain of the ribosomal protein L9, NTL9, from Bacillus stearothermophilus has been monitored by circular dichroism at various temperatures and chemical denaturant concentrations in H2O and D2O. The basic thermodynamic parameters for the unfolding reaction, deltaH(o), deltaS(o), and deltaC(o)p, were determined by global analysis of temperature and denaturant effects on stability. The data were well fit by a model that assumes stability varies linearly with denaturant concentration and that uses the Gibbs-Helmholtz equation to model changes in stability with temperature. The results obtained from the global analysis are consistent with information obtained from individual thermal and chemical denaturations. NTL9 has a maximum stability of 3.78 +/- 0.25 kcal mol(-1) at 14 degrees C. DeltaH(o)(25 degrees C) for protein unfolding equals 9.9 +/- 0.7 kcal mol(-1) and TdeltaS(o)++(25 degrees C) equals 6.2 +/- 0.6 kcal mol(-1). DeltaC(o)p equals 0.53 +/- 0.06 kcal mol(-1) deg(-1). There is a small increase in stability when D2O is substituted for H2O. Based on the results from global analysis, NTL9 is 1.06 +/- 0.60 kcal mol(-1) more stable in D2O at 25 degrees C and Tm is increased by 5.8 +/- 3.6 degrees C in D2O. Based on the results from individual denaturation experiments, NTL9 is 0.68 +/- 0.68 kcal mol(-1) more stable in D2O at 25 degrees C and Tm is increased by 3.5 +/- 2.1 degrees C in D2O. Within experimental error there are no changes in deltaH(o) (25 degrees C) when D2O is substituted for H2O.     

The folding kinetics and thermodynamics of the Fyn-SH3 domain

The equilibrium unfolding and the kinetic folding and unfolding of the 67 residue Fyn-SH3 domain have been investigated. Equilibrium unfolding experiments indicate that, despite the lack of both disulfide bonds and prosthetic groups, Fyn-SH3 is relatively stable with a free energy of folding of -6.0 +/- 0.6 kcal mol-1 at 20 degrees C. Kinetic experiments indicate that the domain refolds in a rapid two-state manner without significant population of intermediates (k = 94.3 s-1 in H2O at 20 degrees C). Despite the presence of two proline residues, the refolding of the domain is monophasic, and no significant proline isomerization-like refolding phase is observed. This can be attributed to an extremely low level of the incorrect (cis) isomer of the structurally important Pro134 residue in the protein denatured in 8 M guanidine hydrochloride. Analysis of the temperature and guanidine hydrochloride dependence of the folding rate suggests that the folding transition state of this protein is relatively well organized. A comparison with the refolding kinetics and thermodynamics of other homologous SH3 domains indicates that these exhibit an equivalent degree of transition state organization. This potentially arises from conservation of key features of the transition state conformation despite sometimes relatively low overall sequence identity. Such a comparison further suggests that relative thermodynamic stability is an important factor in determining the relative folding rates of natural proteins with a common fold, but that specific details of the amino acid sequence can also play a significant role in individual cases.     

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.     

Calorimetry of apolipoprotein-A1 binding to phosphatidylcholine-triolein-cholesterol emulsions

The thermotropic properties of triolein-rich, low-cholesterol dipalmitoyl phosphatidylcholine (DPPC) emulsion particles with well-defined chemical compositions (approximately 88% triolein, 1% cholesterol, 11% diacyl phosphatidylcholine) and particle size distributions (mean diameter, approximately 1000-1100 A) were studied in the absence and presence of apolipoprotein-A1 by a combination of differential scanning and titration calorimetry. The results are compared to egg yolk PC emulsions of similar composition and size. Isothermal titration calorimetry at 30 degrees C was used to saturate the emulsion surface with apo-A1 and rapidly quantitate the binding constants (affinity Ka = 11.1 +/- 3.5 x 10(6) M-1 and capacity N = 1.0 +/- 0.09 apo-A1 per 1000 DPPC) and heats of binding (enthalpy H = -940 +/- 35 kcal mol-1 apo-A1 or -0.92 +/- 0.12 kcal mol-1 DPPC). The entropy of association is -3070 cal deg-1 mol-1 protein or -3 cal deg-1 mol-1 DPPC. Without protein on the surface, the differential scanning calorimetry heating curve of the emulsion showed three endothermic transitions at 24.3 degrees C, 33.0 degrees C, and 40.0 degrees C with a combined enthalpy of 1.53 +/- 0.2 kcal mol-1 DPPC. With apo-A1 on the surface, the heating curve showed the three transitions more clearly, in particular, the second transition became more prominent by significant increases in both the calorimetric and Van't Hoff enthalpies. The combined enthalpy was 2.70 +/- 0.12 kcal mol-1 DPPC and remained constant upon repeated heating and cooling. Indicating that the newly formed DPPC emulsion-Apo-A1 complex is thermally reversible during calorimetry. Thus there is an increase in delta H of 1.17 kcal mol-1 DPPC after apo-A1 is bound, which is roughly balanced by the heat released during binding (-0.92 kcal) of apo-A1. The melting entropy increase, +3.8 cal deg-1 mol-1 DPPC of the three transitions after apo-A1 binds, also roughly balances the entropy (-3 cal deg-1 mol-1 DPPC) of association of apo-A1. These changes indicate that apo-A1 increases the amount of ordered gel-like phase on the surface of DPPC emulsions when added at 30 degrees C. From the stoichiometry of the emulsions we calculate that the mean area of DPPC at the triolein/DPPC interface is 54.5 A2 at 41 degrees C and 54.2 A2 at 30 degrees C. The binding of apo-A1 at 30 degrees C to the emulsion reduces the surface area per DPPC molecule from 54.2 A2 to 50.8 A2. At 30 degrees apo-A1 binds with high affinity and low capacity to the surface of DPPC emulsions and increases the packing density of the lipid domain to which it binds. Apo-A1 was also titrated onto DPPC emulsions at 45 degrees C. This temperature is above the gel liquid crystal transition. No heat was released or adsorbed. Furthermore, egg yolk phosphatidylcholine emulsions of nearly identical composition were also titrated at 30 degrees C with apo-A1 and were euthermic. Association constants were previously measured using a classical centrifugation assay and were used to calculate the entropy of apo-A1 binding (+28 cal deg-1 mol-1 apo-A1). This value indicates that apo-A1 binding to a fluid surface like egg yolk phosphatidylcholine or probably DPPC at 45 degrees C is hydrophobic and is consistent with hydrocarbon lipid or protein moities coming together and excluding water. Thus the binding of apo-A1 to partly crystalline surfaces is entropically negative and increases the order of the already partly ordered phases, whereas binding to liquid surfaces is mainly an entropically driven hydrophobic process.     

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.     

Global analysis of the effects of temperature and denaturant on the folding and unfolding kinetics of the N-terminal domain of the protein L9

The folding and unfolding kinetics of the N-terminal domain of the ribosomal protein L9 have been measured at temperatures between 7 and 85 degrees C and between 0 and 6 M guanidine deuterium chloride. Stopped-flow fluorescence was used to measure rates below 55 degrees C and NMR lineshape analysis was used above 55 degrees C. The amplitudes and rate profiles of the stopped-flow fluorescence experiments are consistent with a two-state folding mechanism, and plots of ln(k) versus guanidine deuterium chloride concentration show the classic v-shape indicative of two-state folding. There is no roll over in the plots when the experiments are repeated in the presence of 400 mM sodium sulfate. Temperature and denaturant effects were fit simultaneously to the simple model k=D exp(-DeltaG*/RT) where DeltaG* represents the change in apparent free energy between the transition state and the folded or unfolded state and D represents the maximum possible folding speed. DeltaG* is assumed to vary linearly with denaturant concentration and the Gibbs-Helmholtz equation is used to model stability changes with temperature. Approximately 60% of the surface area buried upon folding is buried in the transition state as evidenced by changes in the heat capacity and m value between the unfolded state and the transition state. The equilibrium thermodynamic parameters, DeltaCp degrees, m and DeltaG degrees, all agree with the values calculated from the kinetic experiments, providing additional evidence that folding is two-state. The folding rates at 0 M guanidine hydrochloride show a non-Arrhenius temperature dependence typical of globular proteins. When the folding rates are examined along constant DeltaG degrees/T contours they display an Arrhenius temperature dependence with a slope of -8600 K. This indicates that for this system, the non-Arrhenius temperature dependence of folding can be accounted for by the anomalous temperature dependence of the interactions which stabilize proteins.     

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.     

Cold denaturation of ubiquitin

Temperature induced unfolding of bovine ubiquitin in solutions with different concentrations of guanidinium hydrochloride (GdmCl) has been measured using differential scanning calorimetry. It has been shown that at high concentrations of GdmCl the ubiquitin molecule can undergo both heat and cold induced denaturation. Analysis of the enthalpy of unfolding of ubiquitin in the presence of GdmCl shows a good agreement with the thermodynamic denaturant binding model. The unfolding Gibbs energy is found to change linearly with guanidine concentration up to zero denaturant concentration.     

Effect of single and double peptide bond scission by trypsin on the structure and activity of staphylococcal enterotoxin C

Two peptide bonds of staphylococcal enterotoxin C, were hydrolyzed concurrently at quite different rates during limited digestion with trypsin. A Lys-Val at about position 92 in the disulfide loop was the first bond cleaved, followed by a Lys-Asx at about position 57 on the NH2-terminal side of the loop. Preparations of singly cleaved material (enterotoxin C1-T1) contained about 93% of the cleaved protein and 7% unreacted enterotoxin. Preparations of the doubly cleaved material (enterotoxin C1-T2) consisted of 98% enterotoxin C1-T2 and 2% enterotoxin C1-T1. In the absence of denaturant, enterotoxin C1-T2 behaved as a single particle. It gave a single peak on Sephadex G-75 with a sedimentation coefficient of 2.85 S and a molecular weight of 29,100 by sedimentation equilibrium. Circular dichroic spectra indicated only minor conformational differences between enterotoxins C1-T2 and C1. However conformational stability was significantly affected with the unfolding of enterotoxin C1-T2 in 4 M guanidine hydrochloride proceeding at about twice the rate of native enterotoxin. Enterotoxin C1-T2 was separated into 6,500 and 22,000 molecular weight polypeptides by gel filtration on Sepharose 6B in 6 M guanidine hydrochloride. Complementation (as measured by CD spectra, serologic activity and mitogenicity) of the two polypeptides was readily achieved from solution in 6 M guanidine hydrochloride by dialysis against phosphate buffer. The 22,000 molecular weight polypeptide was further separated into two peptides (Mr = 4,000 and 19,000 after alkylation of the reduced disulfide bridge. Summation of the amino acid composition of the constituent peptides of enterotoxin C1-T2 agreed well with the composition of enterotoxin C1. A comparison of the 6,500 and 4,000 molecular weight polypeptides from enterotoxin C1-T2 with structurally equivalent segments of enterotoxin B suggested structural homology between the two antigenic variants. Enterotoxins C1, C1-T1, and C1-T2 gave reactions of complete identity in Ouchterlony immunodiffusion and were indistinguishable in the quantitative precipitin reaction. Enterotoxins C1-T1 and C1-T2 were highly mitogenic but were slightly less potent than the native enterotoxin. Enterotoxin C1-T2 had equivalent emetic activity to enterotoxin C1 in rhesus monkeys. It is suggested that the exceptional lability to limited enzymic hydrolysis exemplified by enterotoxin C1 is associated with beta turn structures at protein surfaces.     

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.     

Refolding rate of stability-enhanced cytochrome c is independent of thermodynamic driving force

N52I iso-2 cytochrome c is a variant of yeast iso-2 cytochrome c in which asparagine substitutes for isoleucine 52 in an alpha helical segment composed of residues 49-56. The N52I substitution results in a significant increase in both stability and cooperativity of equilibrium unfolding, and acts as a "global suppressor" of destabilizing mutations. The equilibrium m-value for denaturant-induced unfolding of N52I iso-2 increases by 30%, a surprisingly large amount for a single residue substitution. The folding/unfolding kinetics for N52I iso-2 have been measured by stopped-flow mixing and by manual mixing, and are compared to the kinetics of folding/unfolding of wild-type protein, iso-2 cytochrome c. The results show that the observable folding rate and the guanidine hydrochloride dependence of the folding rate are the same for iso-2 and N52I iso-2, despite the greater thermodynamic stability of N52I iso-2. Thus, there is no linear free-energy relationship between mutation-induced changes in stability and observable refolding rates. However, for N52I iso-2 the unfolding rate is slower and the guanidine hydrochloride dependence of the unfolding rate is smaller than for iso-2. The differences in the denaturant dependence of the unfolding rates suggest that the N52I substitution decreases the change in the solvent accessible hydrophobic surface between the native state and the transition state. Two aspects of the results are inconsistent with a two-state folding/unfolding mechanism and imply the presence of folding intermediates: (1) observable refolding rate constants calculated from the two-state mechanism by combining equilibrium data and unfolding rate measurements deviate from the observed refolding rate constants; (2) kinetically unresolved signal changes ("burst phase") are observed for both N52I iso-2 and iso-2 refolding. The "burst phase" amplitude is larger for N52I iso-2 than for iso-2, suggesting that the intermediates formed during the "burst phase" are stabilized by the N52I substitution.     

Denaturant m values and heat capacity changes: relation to changes in accessible surface areas of protein unfolding

Denaturant m values, the dependence of the free energy of unfolding on denaturant concentration, have been collected for a large set of proteins. The m value correlates very strongly with the amount of protein surface exposed to solvent upon unfolding, with linear correlation coefficients of R = 0.84 for urea and R = 0.87 for guanidine hydrochloride. These correlations improve to R = 0.90 when the effect of disulfide bonds on the accessible area of the unfolded protein is included. A similar dependence on accessible surface area has been found previously for the heat capacity change (delta Cp), which is confirmed here for our set of proteins. Denaturant m values and heat capacity changes also correlate well with each other. For proteins that undergo a simple two-state unfolding mechanism, the amount of surface exposed to solvent upon unfolding is a main structural determinant for both m values and delta Cp.     

Reduced-denatured ribonuclease A is not in a compact state

Dynamic light scattering and circular dichroism experiments were performed to determine the compactness and residual secondary structure of reduced and by 6 M guanidine hydrochloride denatured ribonuclease A. We find that reduction of the four disulphide bonds by dithiothreitol at 20 degrees C leads to total unfolding and that a temperature increase has no further effect on the dimension. The Stokes' radius of ribonuclease A at 20 degrees C is R(s) = (1.90 +/- 0.04) nm (native) and R(s) = (3.14 +/- 0.06) nm (reduced-denatured). Furthermore, circular dichroism spectra do not indicate any residual secondary structure. We suggest that reduced-denatured Ribonuclease A has a random coil-like conformation and is not in a compact denatured state.     

The equilibrium intermediate of beta-lactoglobulin with non-native alpha-helical structure

It is generally considered that intermediates of protein folding contain partially formed native-like secondary structures. In contrast, we recently reported that the kinetic folding intermediate of bovine beta-lactoglobulin contains non-native alpha-helical structures. To understand the mechanism that stabilizes the non-native intermediate, we characterized by circular dichroism (CD) the equilibrium unfolding transition of beta-lactoglobulin induced by guanidine hydrochloride (Gdn-HCl) at pH 2 and 4 degrees C. The unfolding transition measured by near-UV CD preceded the transition measured by far-UV CD, indicating the accumulation of the intermediate state. The far-UV CD spectrum of the intermediate, obtained by global fitting analysis of the CD spectra in the presence of various concentrations of Gdn-HCl, was similar to the burst-phase intermediate observed in the refolding kinetics, and contained non-native alpha-helical structures. Addition of 10% (v/v) 2,2,2-trifluoroethanol (TFE) increased the helical content of the equilibrium intermediate, although the protein still assumed the native structure in the absence of Gdn-HCl. A phase diagram of the conformational states, i.e. the alpha-helical intermediate, unfolded and native states, against the concentration of TFE and Gdn-HCl was constructed. This indicated that, because of the high helical preference of the amino acid sequence of beta-lactoglobulin, the helical region protrudes into the boundary between the native and unfolded states, resulting in non-monotonic accumulation of the helical intermediate upon equilibrium unfolding of the native beta-sheet structure. This is the first observation to indicate that a non-native alpha-helical intermediate accumulates during equilibrium unfolding of a predominantly beta-sheet protein.