The pH dependence of the reversible unfolding of ovalbumin A1 by guanidine hydrochloride.

The pH dependence of the reversible guanidine hydrochloride denaturation of the major fraction of ovalbumin (ovalbumin A1) was studied by a viscometric method in the pH range 1-7, at 25 degrees C and at six different denaturant concentrations (1.5-2.6 M). At any denaturant concentrationa reduction in pH favoured the transition from the native to the denatured state. The latter was essentially 'structureless', as revealed by the fact that the reduced viscosity of the acid and guanidine hydrochloride denatured state of ovalbumin A1 (obtained at different denaturant concentrations in acidic solutions) was measured (at a protein concentration of 3.8 mg/ml) to be 29.2 ml/g which is identical to that found in 6 M guanidine hydrochloride wherein the protein behaves as a cross-linked random coil. A quantitative analysis of the results on the pH dependence of the equilibrium constant for the denaturation process showed that on denaturation the intrinsic pK of two carboxyl groups in ovalbumin A1 went up from 3.1 in the native state to 4.4 in the denatured state of the protein.     

Dodine as a transparent protein denaturant for circular dichroism and infrared studies

The fungicide dodine combines the cooperative denaturation properties of guanidine with the mM denaturation activity of SDS. It was previously tested only on two small model proteins. Here we show that it can be used as a chemical denaturant for phosphoglycerate kinase (PGK), a much larger two‐domain enzyme. In addition to its properties as a chemical denaturant, dodine facilitates thermal denaturation of PGK, and we show for the first time that it also facilitates pressure denaturation of a protein. Much higher quality circular dichroism and amide I′ infrared spectra of PGK can be obtained in dodine than in guanidine, opening the possibility for use of dodine as a denaturant when UV or IR detection is desirable. One caution is that dodine denaturation, like other detergent‐based denaturants, is less reversible than guanidine denaturation.     

Intrinsic viscosity of ovomucoid in random coil conformation.

Ovomucoid is denatured by concentrated solutions of guanidine hydrochloride. The intrinsic viscosities of the glycoprotein in 6 M guanidine hydrochloride in the absence and presence of beta-mercaptoethanol were found to be 8.1 and 16.0 ml/g, respectively. Ovomucoid with disulphide bonds reduced exists in linear random coil conformation. However, the intrinsic viscosity of the randomly coiled protein was less than that predicted from the empirical equations describing the molecular weight dependence of intrinsic viscosities of random coil proteins in 6 M guanidine hydrochloride. On excluding the carbohydrate content of the protein, which is theoretically justified, the calculated intrinsic viscosity interestingly became closer to the measured one. The temperature dependence of the intrinsic viscosity of ovomucoid in linear random coil conformation was studied in the temperature range, 25-55 degrees. The features of the intrinsic viscosity-temperature profile are not comparable with those exhibited by other linear random coil proteins in 6 M guanidine hydrochloride.     

Infrared spectroscopic discrimination between the loop and alpha-helices and determination of the loop diffusion kinetics by temperature-jump time-resolved infrared spectroscopy for cytochrome c

The infrared (IR) absorption of the amide I band for the loop structure may overlap with that of the alpha-helices, which can lead to the misassignment of the protein secondary structures. A resolution-enhanced Fourier transform infrared (FTIR) spectroscopic method and temperature-jump (T-jump) time-resolved IR absorbance difference spectra were used to identify one specific loop absorption from the helical IR absorption bands of horse heart cytochrome c in D2O at a pD around 7.0. This small loop consists of residues 70-85 with Met-80 binding to the heme Fe(III). The FTIR spectra in amide I' region indicate that the loop and the helical absorption bands overlap at 1653 cm(-1) at room temperature. Thermal titration of the amide I' intensity at 1653 cm(-1) reveals that a transition in loop structural change occurs at lower temperature (Tm=45 degrees C), well before the global unfolding of the secondary structure (Tm approximately 82 degrees C). This loop structural change is assigned as being triggered by the Met-80 deligation from the heme Fe(III). T-jump time-resolved IR absorbance difference spectra reveal that a T-jump from 25 degrees C to 35 degrees C breaks the Fe-S bond between the Met-80 and the iron reversibly, which leads to a loop (1653 cm(-1), overlap with the helical absorption) to random coil (1645 cm(-1)) transition. The observed unfolding rate constant interpreted as the intrachain diffusion rate for this 16 residue loop was approximately 3.6x10(6) s(-1).     

A compact monomeric intermediate identified by NMR in the denaturation of dimeric triose phosphate isomerase

The denaturation of triose phosphate isomerase (TIM) from Saccharomyces cerevisiae by guanidine hydrochlorids at pH 7.2 has been monitored by NMR spectroscopy in conjunction with optical spectroscopy. In the absence of denaturant, the hydrodynamic radius of 29.6(+/-0.25) A and the substantial chemical shift dispersion evident in the NMR spectrum are consistent with the highly structured dimeric native state of the protein. On the addition of 2. 2 M guanidine hydrochloride the effective hydrodynamic radius increases to 51.4(+/-0.43) A, consistent with that anticipated for the polypeptide chain in a highly unstructured random coil state. In 1.1 M guanidine hydrochloride, however, the effective hydrodynamic radius is 24.0(+/-0.25) A, a value substantially decreased relative to that of the native dimeric state but very close to that anticipated for a monomeric species with native-like compaction (23. 5 A). The lack of chemical shift dispersion indicates, however, that few tertiary interactions persist within this species. Far UV CD and intrinsic fluorescence measurements show that this compact intermediate retains significant secondary structure and that on average the fluorophores are partially excluded from solvent. Such a species could be important in the formation of dimeric TIM from its unfolded state.     

A guanidine hydrochloride induced change in ribonuclease without gross unfolding

Although denaturation of ribonuclease by guanidine hydrochloride to a random coil has been considered to be a simple two-state mechanism, the time dependence of our calorimetric data indicate that a cooperative endothermic pretransition may occur near 1.25 M. guanidine hydrochloride (pH 6 and 25°C) without gross unfolding of the protein. Reexamination of other observables as a function of guanidine hydrochloride concentrations as well as activity measurements suggests the possibility of some process other than simple binding occurring in the concentration range below the onset of gross denaturation.     

Subunit dissociation and unfolding of rabbit muscle phosphofructokinase by guanidine by hydrochloride.

The denaturation of rabbit skeletal muscle phosphofructokinase by guanidine hydrochloride has been studied using fluorescence, light scattering, and enzyme activity measurements. The transition from fully active tetramer (0.1 M potassium phosphate (pH 8.0) at 10 and 23 degrees) to unfolded polypeptide chains occurs in two phases as measured by changes in the fluorescence spectrum and light scattering of the protein: dissociation to monomers at low guanidine hydrochloride concentrations (similar to 0.8 M) followed by an unfolding of the polypeptide chains, which presumably results in a random coil state, at high concentrations of denaturant (greater than 3.5 M). The initial transition can be further divided into two distinct stages. The native enzyme is rapidly dissociated to inactive monomers which then undergo a much slower conformational change that alters the fluorescence spectrum of the protein. The dissociation is complete within 2 min and is reversible, but the conformational change requires about 2 hr for completion and is not reversible under a variety of conditions, including the presence of substrates and allosteric effectors. The conformationally altered protomer reaggregates to form a precipitate at 23 degrees, but is stable below 10 degrees. The second major phase of the denaturation is fully reversible. A simple mechanism is proposed to account for the results, and its implications for the corresponding renaturation process are discussed.     

Circular dichroism and gel filtration behavior of subtilisin enzymes in concentrated solutions of guanidine hydrochloride.

The circular dichroism of diisopropylphosphorylsubtilisins Novo and Carlsberg in both the near- and farultraviolet spectral regions is unaltered by concentrations of guanidine hydrochloride as high as 4 M at neutral pH. At concentrations of guanidine hydrochloride greater than 4 M slow irreversible time-dependent changes, apparently obeying second-order kinetics, are evident in both the near- and far-ultraviolet circular dichroism of these enzymes. Gel filtration studies of inactivated subtilisin enzymes reveal the circular dichroism changes to be accompained by the appearance of aggregated protein material. The changes in circular dichroism and the production of associated subtilisin species are sensitive to protein concentration, denaturant concentrations, and pH. The circular dichroism of active subtilisins Novo and Carlsberg in guanidine hydrochloride exhibits irreversible changes similar to those observed for the inactivated subtilisins. Aggregated protein material is also formed initially in the presence of guanidine hydrochloride, but is rapidly autolyzed to low molecular weight fragments.     

Denaturation of thymidylate synthetase from amethopterin-resistant Lactobacillus casei.

The effects of various concentrations of urea and guanidine hydrochloride on enzyme activity and on subunit association were determined. Incubation of thymidylate synthetase with buffered solutions of 3M to 3.5M guanidine hydrochloride or 5 M to 6 M urea resulted in the loss of about 90% of the enzyme activity. Under these denaturing conditions a red shift of the fluorescence emission maximum from 340 nm to 351 nm was observed together with a significant decrease in the relative fluorescence intensity of the protein. Studies at both 4 degrees C and 25 degrees C indicated that the enzyme was in the dimer form in 2 M guanidine hydrochloride but was dissociated into monomers in concentrations of this denaturant of 3 M and above. Although only monomeric species were evident at 4 degrees C in 6 M urea, at 25 25 degrees C this denaturant caused protein aggregation which increased with decreasing phosphate buffer concentration. Enzyme (5 mg/ml) in 0.5 M potassium phosphate buffer, pH 6.8, containing 4 M guanidine hydrochloride gave a minimum S20, w value of 1.22S at 25 degrees C. Sedimentation behavior of the native enzyme in the range of 5 to 20 mg/ml was only slightly concentration-dependent (4.28 S to 4.86 S) but extensive aggregation occurred above 20 mg/ml.     

Small-angle X-ray scattering and single-molecule FRET spectroscopy produce highly divergent views of the low-denaturant unfolded state

The results of more than a dozen single-molecule F?rster resonance energy transfer (smFRET) experiments suggest that chemically unfolded polypeptides invariably collapse from an expanded random coil to more compact dimensions as the denaturant concentration is reduced. In sharp contrast, small-angle X-ray scattering (SAXS) studies suggest that, at least for single-domain proteins at non-zero denaturant concentrations, such compaction may be rare. Here, we explore this discrepancy by studying protein L, a protein previously studied by SAXS (at 5?°C), which suggested fixed unfolded-state dimensions from 1.4 to 5?M guanidine hydrochloride (GuHCl), and by smFRET (at 25?°C), which suggested that, in contrast, the chain contracts by 15-30% over this same denaturant range. Repeating the earlier SAXS study under the same conditions employed in the smFRET studies, we observe little, if any, evidence that the unfolded state of protein L contracts as the concentration of GuHCl is reduced. For example, scattering profiles (and thus the shape and dimensions) collected within ～4?ms after dilution to as low as 0.67?M GuHCl are effectively indistinguishable from those observed at equilibrium at higher denaturant. Our results thus argue that the disagreement between SAXS and smFRET is statistically significant and that the experimental evidence in favor of obligate polypeptide collapse at low denaturant cannot be considered conclusive yet.     

Reversible dissociation and unfolding of aspartate aminotransferase from Escherichia coli: characterization of a monomeric intermediate

The unfolding and dissociation of the dimeric enzyme aspartate aminotransferase (D) from Escherichia coli by guanidine hydrochloride have been investigated at equilibrium. The overall process was reversible, as judged from almost complete recovery of enzymic activity after dialysis of 0.7 mg of denatured protein/mL against buffer. Unfolding and dissociation were monitored by circular dichroism and fluorescence spectroscopy and occurred in three separate phases: D in equilibrium 2M in equilibrium 2M* in equilibrium 2U. The first transition at about 0.5 M guanidine hydrochloride coincided with loss of enzyme activity. It was displaced toward higher denaturant concentrations by the presence of either pyridoxal 5'-phosphate or pyridoxamine 5'-phosphate and toward lower denaturant concentrations by decreasing the protein concentration. Therefore, bound coenzyme stabilizes the dimeric state, and the monomer (M) is inactive because the shared active sites are destroyed by dissociation of the dimer. M was converted to M* and then to the fully unfolded monomer (U) in two subsequent transitions. M* was stable between 0.9 and 1.1 M guanidine hydrochloride and had the hydrodynamic radius, circular dichroism, and fluorescence of a monomeric, compact "molten globule" state.     

Conformational properties of the iso-1-cytochrome C denatured state: dependence on guanidine hydrochloride concentration

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

Determination of the secondary structure of proteins from the amide I band of the laser Raman spectrum

The amide I band in the laser Raman spectrum of proteins has been resolved into six components, each representing residues in a different type of secondary structure. These structure types are ordered or bihydrogen-bonded helix (believed to be located in the center of helical segments), disordered or monohydrogen-bonded helix (believed to be located at the ends of helical segments), antiparallel beta sheet, parallel beta sheet, reverse turn, and undefined. The Raman spectrum representing 100% of each type of residue conformation has been computed from the solvent-subtracted Raman spectra of ten proteins with known secondary structure, plus poly-l-lysine using a least-squares solution of the overdetermined system of equations. Linear combinations of these reference spectra were then fitted to the experimental amide I spectra of these and other proteins to estimate the fractions of residues in these conformations. Statistical tests suggest that the discrimination between bihydrogen-bonded helix and monohydrogen-bonded helix is significant as is the discrimination between parallel and antiparallel β-sheet. However, the discrimination between random structure and turns has not yet been accomplished by these studies. The absolute difference between X-ray and Raman estimates of structure for 17 protein samples is generally less than 6%. We conclude that detailed and reasonably accurate estimates of secondary structure can be derived from the amide I spectra of proteins.     

Secondary structure of calsequestrin in solutions and in crystals as determined by Raman spectroscopy

Calsequestrin has been precipitated with calcium into five different crystal forms: cruciform twins, flat rectangles, thin needles, bipyramids, rectangular prisms, and a sixth precrystalline form, spheres. Raman spectra of the spheres and the cruciform twins are the same. The Raman spectrum of a physiological concentration (10%) of calsequestrin in calcium-free solution is the same as the spectrum of calcium precipitated calsequestrin in the amide I region, and in the C-C stretching region, but these spectra are different in the amide III region. The Raman spectrum of unfolded calsequestrin in 5 M guanidine hydrochloride is quite different from the other spectra, but it is not similar to the spectra of other unfolded proteins. Estimates of secondary structure from the amide I region indicate that calsequestrin in calcium-free solution and calcium-precipitated forms has 40 +/- 5% helix, 30 +/- 4% beta-strand, and 18 +/- 2% reverse turn. Secondary structure estimates calculated from the amide III region are not significantly different. They indicate 41 +/- 5% helix and 36 +/- 6% beta-strand for the precipitated forms, and 32 +/- 5% helix and 39 +/- 6% beta-strand for solutions. Calsequestrin unfolded in 5 M guanidine hydrochloride at 100 mg/ml gives 24 +/- 5% helix and 48 +/- 6% beta-strand.     

Measuring unfolding of proteins in the presence of denaturant using fluorescence correlation spectroscopy

IFABP is a small (15 kDa) protein consisting mostly of antiparallel beta-strands that surround a large cavity into which ligands bind. We have previously used FCS to show that the native protein, labeled with fluorescein, exhibits dynamic fluctuation with a relaxation time of 35 micros. Here we report the use of FCS to study the unfolding of the protein induced by guanidine hydrochloride. Although the application of this technique to measure diffusion coefficients and molecular dynamics is straightforward, the FCS results need to be corrected for both viscosity and refractive index changes as the guanidine hydrochloride concentration increases. We present here a detailed study of the effects of viscosity and refractive index of guanidine hydrochloride solutions to calibrate FCS data. After correction, the increase in the diffusion time of IFABP corresponds well with the unfolding transition monitored by far ultraviolet circular dichroism. We also show that the magnitude of the 35 micros phase, reflecting the conformational fluctuation in the native state, decreases sharply as the concentration of denaturant increases and the protein unfolds. Although FCS experiments indicate that the unfolded state at pH 2 is rather compact and native-like, the radius in the presence of guanidine hydrochloride falls well within the range expected for a random coil.     

Structural studies of apolipoprotein B: physical properties of the protein in guanidine hydrochloride

Apolipoprotein B was isolated from human plasma low-density-lipoprotein without precipitation by diethyl ether/ethanol extraction of the protein in 6 M guanidine hydrochloride. The physical properties of this protein, which contained a residuum of approximately 7% phospholipid, were examined in 6 M guanidine solution under reducing conditions. The circular dichroism spectrum was indistinguishable from that of a random coil protein. Sedimentation equilibrium analyses of apolipoprotein B by the meniscus depletion method of Yphantis (1984, Biochemistry 3, 297-317) were complicated by heterogeneity and nonideality despite the low concentrations employed. 63 analyses of the weight average (Mw) and z average (Mz) molecular weight were made on the apolipoprotein B from 12 subjects. The Mw observed was a function of initial concentration, rotor speed, and a heterogeneity index (Mz/Mw). Multiple linear regression of apolipoprotein B molecular mass against these parameters suggested that an Mw of 540,000 +/- 110,000 would be observed under apparently ideal and homogeneous conditions. The sedimentation coefficient and intrinsic viscosity of the reduced protein at 25 degrees C in 6 M guanidine were 2.13 S and 116 ml/g, respectively; these values predict molecular weights of 640,000 and 250,000, respectively, if apolipoprotein B was fully denatured into a random coil. Lack of agreement between these estimates and with the sedimentation equilibrium analysis can best be explained by compactness of structure and incomplete denaturation to a random coil state. Furthermore, an irreversible temperature dependence of apolipoprotein B reduced viscosity indicated that residual structure remained in solutions of 6 M guanidine hydrochloride/20 mM dithiothreitol. Taken together, the physical data demonstrate that apolipoprotein is a single polypeptide of approximately 540 kDa, whose structure resists denaturation under conditions where most proteins exist as random coils.     

The effects of anions on the solution structure of Na,K-ATPase

Anions interact with protein to induce structural changes at ligand binding sites. The effects of anion complexation include structural stabilization and promote cation-protein interaction. This study was designed to examine the interaction of aspirin and ascorbate anions with the Na+, K+-dependent adenosine triphosphatase (Na,K-ATPase) in H2O and D2O solutions at physiological pH, using anion concentrations of 0.1 microM to 1 mM with final protein concentration of 0.5 to 1 mg/ml. Absorption spectra and Fourier transform infrared (FTIR) difference spectroscopy with its self-deconvolution, second derivative resolution enhancement and curve-fitting procedures were applied to characterize the anion binding mode, binding constant, and the protein secondary structure in the anion-ATPase complexes. Spectroscopic evidence showed that the anion interaction is mainly through the polypeptide C=O and C-N groups with minor perturbation of the lipid moiety. Evidence for this came from major spectral changes (intensity variations) of the protein amide I and amide II vibrations at 1651 and 1550 cm(-1). respectively. The anion-ATPase binding constants were K=6.45 x 10(3) M(-1) for aspirin and K=1.04 x 10(4) M(-1) for ascorbate complexes. The anion interaction resulted in major protein secondary structural changes from that of the alpha-helix 19.8%; beta-pleated sheet 25.6%; turn 9.1%; beta-antiparallel 7.5% and random 38% in the free Na,K-ATPase to that of the alpha-helix 24-26%; beta-pleated 17-18%; turn 8%; beta-antiparallel 5-3% and random 45.0% in the anion-ATPase complexes.     

Guanidine-induced dissociation of mitochondrial F1-ATPase

The effect of guanidine hydrochloride on ATPase activity, gel filtration, turbidity, and the fluorescence emission intensity of mitochondrial F1-ATPase was examined. Purified F1 from bovine heart mitochondria was slowly inactivated at low denaturant concentration, and inactivation was associated with delta and epsilon subunit dissociation. delta and epsilon subunits were bound together to form a stable and soluble heterodimer. In parallel, appearance of turbidity was observed. This was caused by the formation of alpha3beta3gamma non-covalent aggregates, as analyzed by SDS-PAGE. Short periods of exposition of the F1 complex to high concentrations of guanidine hydrochloride (0.8-3 M) again induced deltaepsilon dissociation as a heterodimer and the formation of an inactive alpha3beta3gamma subcomplex. This eventually dissociated progressively into single subunits caused by partial unfolding, as evidenced through changes of the protein intrinsic fluorescence emission. Our results suggest that the delta and epsilon subunits are loosely bound to alpha3beta3gamma , and play an important role in determining structural stability to isolated mitochondrial F1-ATPase.     

Partial specific volumes and interactions with solvent components of α-globulin fromSesamum indicum L. in urea and guanidine hydrochloride

The interaction of α-globulin with urea/guanidine hydrochloride was investigated by determining the apparent partial specific volumes of the protein in these solvents. The apparent partial specific volumes were determined both under isomolal and isopotential conditions. The preferential interaction parameter with solvent components calculated were 0.08 and 0.1 g of urea and guanidine hydrochloride respectively per g protein. In both the cases the interaction was not preferential with water. The total binding of denaturant to α-globulin was calculated both for urea and guanidine hydrochloride and the correlation between experimentally determined number of mol of denaturant bound per mol of protein and the total number of peptide bonds and aromatic amino acids were found to be in excellent agreement with each other. The changes in volume upon transferring α-globulin from a salt solution to 8 M urea and 6 M guanidine hydrochloride were also calculated. This work was done at the Biochemistry Department, Brandeis University, Waltham, Massachusetts 02254, USA.     

Protein stabilization by urea and guanidine hydrochloride

The urea, guanidine hydrochloride, salt, and temperature dependence of the rate of dissociation of CO from a nonequilibrium state of CO-bound native ferrocytochrome c has been studied at pH 7. The heme iron of ferrocytochrome c in the presence of denaturing concentrations of guanidine hydrochloride (GdnHCl) and urea prepared in 0.1 M phosphate, pH 7, binds CO. When the unfolded protein solution is diluted 101-fold into CO-free folding buffer, the protein chain refolds completely, leaving the CO molecule bonded to the heme iron. Subsequently, slow thermal dissociation of the CO molecule yields to the heme coordination of the native M80 ligand. Thus, the reaction monitors the rate of thermal conversion of the CO-liganded native ferrocytochrome c to the M80-liganded native protein. The rate of this reaction, k(diss), shows a characteristic dependence on the presence of nondenaturing concentrations of the denaturants in the reaction medium. The rate decreases by approximately 1.9-3-fold as the concentration of GdnHCl in the refolding medium increases from nearly 0 to approximately 2.1 M. Similarly, the rate decreases by 1.8-fold as the urea concentration is raised from 0.l to approximately 5 M. At still higher concentrations of the denaturants the denaturing effect sets in, the protein is destabilized, and hence the CO dissociation rate increases sharply. The activation energy of the reaction, E(a), increases when the denaturant concentration in the reaction medium is raised: from 24.1 to 28.3 kcal mol(-1) for a 0.05-2.1 M rise in GdnHCl and from 25.2 to 26.9 kcal mol(-1) for a 0.1-26.9 M increase in urea. Corresponding to these increases in denaturant concentrations are also increases in the activation entropy, S(diss)/R, where R is the gas constant of the reaction. The denaturant dependence of these kinetic and thermodynamic parameters of the CO dissociation reaction suggests that binding interactions with GdnHCl and urea can increase the structural and energetic stability of ferrocytochrome c up to the limit of the subdenaturing concentrations of the additives. NaCl and Na(2)SO(4), which stabilize proteins through their salting-in effect, also decrease the rate with a corresponding increase in activation entropy of CO dissociation from CO-bound native ferrocytochrome c, lending support to the view that low concentrations of GdnHCl and urea stabilize proteins. These results have direct relevance to the understanding and interpretation of the free energy-denaturant relationship and protein folding chevrons.