Effects of guanidine hydrochloride on the refolding kinetics of denatured thioredoxin

The effect of guanidine hydrochloride concentration on the kinetics of the conformational change of Escherichia coli thioredoxin was examined by using fluorescence, absorbance, circular dichroic, and viscosity measurements. Native thioredoxin unfolds in a single kinetic phase whose time constant decreases markedly with increasing denaturant concentration in the denaturation base-line zone. This dependency merges with the time constant of the slowest refolding kinetic phase at the midpoint of the equilibrium transition in 2.5 M denaturant. The time constant of the slowest refolding phase becomes denaturant independent below 1 M denaturant in the native base-line region. The denaturant-independent slowest refolding phase has an activation energy of 16 kcal/mol and is generated in the denatured base-line zone in a denaturant-independent reaction having a time constant of 19 s at 25 degrees C. The fractional amplitude of the slowest refolding phase diminishes in the native base-line zone to a minimum value of 0.25. This decrease is accompanied by an increase in the fractional amplitudes of two faster refolding kinetic phases, an increase describing a sigmoidal transition centered at about 1.6 M denaturant. Manual multimixing measurements indicate that only the slowest refolding kinetic phase generates a product having the stability of the native protein. We suggest that the two faster refolding phases reflect the transient accumulation of folding intermediates which can contain a nonnative isomer of proline peptide 76.     

Conformational transitions of thioredoxin in guanidine hydrochloride

Spectral and hydrodynamic measurements of thioredoxin from Escherichia coli indicate that the compact globular structure of the native protein is significantly unfolded in the presence of guanidine hydrochloride concentrations in excess of 3.3 M at neutral pH and 25 degrees C. This conformational transition having a midpoint at 2.5 M denaturant is quantitatively reversible and highly cooperative. Stopped-flow measurements of unfolding in 4 M denaturant, observed with tryptophan fluorescence as the spectral probe, reveal a single kinetic phase having a relaxation time of 7.1 +/- 0.2 s. Refolding measurements in 2 M denaturant reveal three kinetic phases having relaxation times of 0.54 +/- 0.23, 14 +/- 6, and 500 +/- 130 s, accounting for 12 +/- 2%, 10 +/- 1%, and 78 +/- 3% of the observed change in tryptophan fluorescence. The dominant slowest phase is generated in the denatured state with a relaxation time of 42 s observed in 4 M denaturant. Both the slowest phase observed in refolding and the generation of the slowest phase in the denatured state have an activation enthalpy of 22 +/- 1 kcal/mol. These features of the slowest phase are compatible with an obligatory peptide isomerization of proline-76 to its cis isomer prior to refolding.     

Refolding of denatured ribonuclease observed by size exclusion chromatography

The unfolding and refolding of pancreatic ribonuclease have been observed by absorbance, fluorescence, and size exclusion chromatographic measurements in solutions of guanidinium chloride continuously maintained at pH 6.0 and 4 degrees C. The spectral measurements were fitted with a minimal number of kinetic phases while the chromatographic measurements were simulated from an explicit mechanism. All of the measurements are consistent with a minimal mechanism involving seven components. The folded components include the native protein and two transiently stable intermediates each having the same hydrodynamic volume. The intermediate having all native peptide isomers has an unfolding midpoint in 3.8 M denaturant while the intermediate having one nonnative peptide isomer has an unfolding midpoint in 1.3 M denaturant. The unfolded protein is distributed among four components having the same hydrodynamic volume but differing peptide isomers. At equilibrium, 10% of the denatured protein has all native isomers, 60% has one nonnative isomer, 5% has a different nonnative isomer, and 25% has both nonnative isomers. In low denaturant concentrations, the dominant component with one nonnative isomer can refold to transiently populate the compact intermediate with the same nonnative isomer.     

Equilibrium and kinetic measurements of the conformational transition of reduced thioredoxin

The single disulfide bond in Escherichia coli thioredoxin was reduced by reaction with a 20-fold excess of reduced dithiothreitol at neutral pH and 25 degrees C. For some measurements, reduced thioredoxin was further reacted with iodoacetamide to alkylate the cysteinyl residues. The denaturation transitions of oxidized, reduced, and reduced alkylated thioredoxin were observed by using far-ultraviolet circular dichroic and exclusion chromatographic measurements. Cleavage of the disulfide bond lowers the stability of the native thioredoxin to denaturation by about 2.4 kcal/mol, and subsequent alkylation lowers the stability by a further 1.6 kcal/mol. The kinetics of the conformational change of reduced thioredoxin in guanidine hydrochloride were observed by using exclusion chromatography at moderate pressure and 2 degrees C. Analyses of single and multimixing protocols are consistent with a predominant nonnative configuration in the denatured state and the transient accumulation of a compact nativelike intermediate during refolding. The intermediate can incorporate the nonnative configuration and can accommodate its isomerization. No compelling chromatographic evidence was found for a conformation having an elution time different from that characteristic for either the native or the denatured protein.     

Effects of guanidine hydrochloride on the proton inventory of proteins: implications on interpretations of protein stability

The DeltaG degrees (N)(-)(D) value obtained from extrapolation to zero denaturant concentration by the linear extrapolation method (LEM) is commonly interpreted to represent the Gibbs energy difference between native (N) and denatured (D) ensembles at the limit of zero denaturant concentration. For DeltaG degrees (N)(-)(D) to be interpreted solely in terms of N and D, as is common practice, it must be shown to be independent of denaturant concentration. Because DeltaG degrees (N)(-)(D) is often observed to be dependent on the nature of the denaturant, it is necessary to determine the circumstances under which DeltaG degrees (N)(-)(D) can be interpreted as a property solely of the protein. Here, we use proton inventory, a thermodynamic property of both the native and denatured ensembles, to monitor the thermodynamic character of denaturant-dependent aspects of N and D ensembles and the N right arrow over left arrow D transition. Use of a thermodynamic rather than a spectral parameter to monitor denaturation provides insight into the manner in which denaturant affects the meaning of DeltaG degrees (N)(-)(D) and the nature of the N right arrow over left arrow D transition. Three classes of proteins are defined in terms of the thermodynamic behaviors of their N right arrow over left arrow D transition and N and D ensembles. With guanidine hydrochloride as a denaturant, the classification of protein denaturations by these procedures determines when the LEM gives readily interpretable DeltaG degrees (N)(-)(D) values with this denaturant and when it does not.     

Structural transitions of soluble and immobilized chymotrypsinogen A in urea and guanidinium chloride as measured by fluorescence

A cylindrical flow-through quartz cell was designed for measuring fluorescence changes associated with structural transitions in proteins immobilized by covalent attachment to insoluble matrices. Chymotrypsinogen A was immobilized by covalent attachment to derivatized porous glass beads. Conformational transitions in both native, soluble chymotrypsinogen and glass-bound chymotrypsinogen were assessed from fluorescence emission spectra obtained in 0 to 8 m urea and in 0 to 7 m guanidinium chloride. Evidence for the complete reversibility of such transitions in this zymogen was provided by comparing spectra generated by the native zymogen exposed to a given concentration of denaturant with spectra recorded for a mixture of the native zymogen and completely denatured zymogen at the same final concentration of denaturant. The observed transition appeared to follow a two-state mechanism. First order kinetics of unfolding and of refolding were observed in the transition region of the immobilized protein by monitoring fluorescence changes after rapidly adjusting the concentration of denaturant; apparent first order rate constants at pH 7 and 25 °C averaged 0.016 min^?1. Neither the chemistry of the immobilization reactions nor the microenvironment of the surface appears to affect the stability of the native zymogen or the refolding of denatured chymotrypsinogen. Thus, it appears that immobilization of proteins can provide a means for investigating conformational transitions which, due to such complicating secondary reactions as protein-protein interactions and autolysis, cannot otherwise be examined.     

Chromatographic methods for the isolation of,and refolding of proteins from,Escherichia coli inclusion bodies

New methods for the chromatographic isolation of inclusion bodies directly from crude Escherichia coli homogenates and for the refolding of denatured protein are presented. The traditional method of differential centrifugation for the isolation of purified inclusion bodies is replaced by a single gel-filtration step. The principle is that the exclusion limit of the gel particles is chosen such that only the inclusion bodies are excluded, i.e., all other components of the crude homogenate penetrate the gel under the conditions selected. In the novel column refolding process, a decreasing gradient of denaturant (urea or Gu-HCl), combined with an increasing pH gradient, is introduced into a gel-filtration column packed with a gel medium that has an exclusion limit lower than the molecular mass of the protein to be refolded. A limited sample volume of the protein, dissolved in the highest denaturant concentration at the lowest pH of the selected gradient combination, is applied to the column. During the course of elution, the zone of denatured protein moves down the column at a speed approximately threefold higher than that of the denaturant. This means that the protein sample will gradually pass through areas of increasingly lower denaturant concentrations and higher pH, which promotes refolding into the native conformation. The shape and slope of the gradients, as well as the flow rate, will influence the refolding rate and can be adjusted for different protein samples. The principle is illustrated using a denatured recombinant scFv fusion protein obtained from E. coli inclusion bodies.     

Structural thermodynamics of a random coil protein in guanidine hydrochloride

An important problem in protein folding is to understand the relationship between the structure of a denatured ensemble and its thermodynamics. Using 0 – 6M GdnHCl at fixed pH, we evaluated dimensional changes of an extensively denatured ensemble along with a thermodynamic parameter (Δυ) that monitors the proton inventory of the ensemble. Reduced and carboxyamidated ribonuclease A (RCAM) is a member of a class of disulfide‐free RNase A molecules believed to be random coils (extensively denatured) in aqueous solution. Because GdnHCl interacts more favorably with the protein than water does, this denaturant is observed to increase the Stokes radius of the random coil, with the greatest Stokes radius change occurring in the 0 – 1.5M GdnHCl range. Measurement of the degree of protonation (proton inventory) of the ensemble as a function of GdnHCl at the fixed pH shows that the thermodynamic character of the ensemble also changes markedly in the 0 – 1.5M GdnHCl range, but with little or no change beyond 1.5M GdnHCl. To obtain denaturant‐independent ΔG°_N–D values, the linear extrapolation method (LEM) requires the thermodynamic character of the native and denatured ensembles to be invariant in the transition zone. The results reported here indicate that proteins with a transition midpoint in the 0 – 1.5M GdnHCl range will not give denaturant‐concentration independent ΔG°_N–D values. Such LEM‐derived ΔG°_N–D quantities are a property of the protein and the denaturant, a condition that considerably limits their value in understanding structural energetics. Proteins 2000;41:44–49. © 2000 Wiley‐Liss, Inc.     

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.     

Characterization of the denatured states distribution of neocarzinostatin by small-angle neutron scattering and differential scanning calorimetry

The denatured states of a small globular protein, apo-neocarzinostatin (NCS), have been characterized using several techniques. Structural properties were investigated by optical spectroscopy techniques and small-angle neutron scattering (SANS), as a function of guanidinium chloride (GdmCl) concentration. SANS experiments show that in heavy water, the protein keeps its native size at GdmCl concentrations below 2.5 M. A sharp transition occurs at about 3.6 M GdmCl, and NCS behaves like an excluded volume chain above 5 M. The same behavior is observed in deuterated buffer by fluorescence and circular dichroism measurements. For the H(2)O buffer, the transition occurs with lower concentration of denaturant, the shift being about 0.6 M. 8-Anilino-1-naphthalenesulfonate (ANS) was used as a hydrophobic fluorescent probe for studying the early stages of protein unfolding. Protein denaturation modifies the fluorescence intensity of ANS, a maximum of intensity being detected close to 2 M GdmCl in hydrogenated buffer, which shows the existence of at least one intermediate state populated at the beginning of the unfolding pathway. Differential scanning calorimetry (DSC) was used to obtain thermodynamic values for NCS denaturation. The melting curves recorded between 20 and 90 degrees C in the presence of various GdmCl concentrations (0-3 M) cannot be explained by a simple two-state model. Altogether, the data presented in this paper suggest that before unfolding the protein explores a distribution of states which is centered around compact states at denaturant concentrations below 2 M in H(2)O, and then shifts to less structured states by increasing denaturant concentrations.     

Folding pathway of FKBP12 and characterisation of the transition state.

The folding pathway of human FKBP12, a 12 kDa FK506-binding protein (immunophilin), has been characterised. Unfolding and refolding rate constants have been determined over a wide range of denaturant concentrations and data are shown to fit to a two-state model of folding in which only the denatured and native states are significantly populated, even in the absence of denaturant. This simple model for folding, in which no intermediate states are significantly populated, is further supported from stopped-flow circular dichroism experiments in which no fast "burst" phases are observed. FKBP12, with 107 residues, is the largest protein to date which folds with simple two-state kinetics in water (kF=4 s(-1)at 25 degrees C). The topological crossing of two loops in FKBP12, a structural element suggested to cause kinetic traps during folding, seems to have little effect on the folding pathway.The transition state for folding has been characterised by a series of experiments on wild-type FKBP12. Information on the thermodynamic nature of, the solvent accessibility of, and secondary structure in, the transition state was obtained from experiments measuring the unfolding and refolding rate constants as a function of temperature, denaturant concentration and trifluoroethanol concentration. In addition, unfolding and refolding studies in the presence of ligand provided information on the structure of the ligand-binding pocket in the transition state. The data suggest a compact transition state relative to the unfolded state with some 70 % of the surface area buried. The ligand-binding site, which is formed mainly by two loops, is largely unstructured in the transition state. The trifluoroethanol experiments suggest that the alpha-helix may be formed in the transition state. These results are compared with results from protein engineering studies and molecular dynamics simulations (see the accompanying paper).     

Structural dynamics, stability and folding of proteins

The present concepts of protein folding in vitro are reviewed. According to these concepts, amino acid sequence of protein, which has appeared a result of evolutionary selection, determines the native structure of protein, the pathway of protein folding, and the existence of free energy barrier between native and denatured states of protein. The latter means that protein macromolecule can exist in either native or denatured state. And all macromolecules in the native state are identical but for structural fluctuations due to Brownian motion of their atoms. Identity of all molecules in native state is of primary importance for their correct functioning. The dependence of protein stability, which is measured as the difference between free energy of protein in native and denatured states, on temperature and denaturant concentration is discussed. The modern approaches characterizing transition state and nucleation are regarded. The role of intermediate and misfolded states in amorphous aggregate and amyloid fibril formation is discussed.     

Metal ion-induced stabilization and refolding of anticoagulation factor II from the venom of Agkistrodon acutus

Anticoagulation factor II (ACF II) isolated from the venom of Agkistrodon acutus is an activated coagulation factor X-binding protein in a Ca(2+)-dependent fashion with marked anticoagulant activity. The equilibrium unfolding/refolding of apo-ACF II, holo-ACF II, and Tb(3+)-reconstituted ACF II in guanidine hydrochloride (GdnHCl) solutions was studied by following the fluorescence and circular dichroism (CD). Metal ions were found to increase the structural stability of ACF II against GdnHCl and irreversible thermal denaturation and, furthermore, influence its unfolding/refolding behavior. The GdnHCl-induced unfolding/refolding of both apo-ACF II and Tb(3+)-ACF II is a two-state process with no detectable intermediate state, while the GdnHCl-induced unfolding/refolding of holo-ACF II in the presence of 1 mM Ca(2+) follows a three-state transition with an intermediate state. Ca(2+) ions play an important role in the stabilization of both native and I states of holo-ACF II. The decalcification of holo-ACF II shifts the ending zone of unfolding/refolding curve toward lower GdnHCl concentration, while the reconstitution of apo-ACF II with Tb(3+) ions shifts the initial zone of the denaturation curve toward higher GdnHCl concentration. Therefore, it is possible to find a denaturant concentration (2.1 M GdnHCl) at which refolding from the fully denatured state of apo-ACF II to the I state of holo-ACF II or to the native state of Tb(3+)-ACF II can be initiated merely by adding the 1 mM Ca(2+) ions or 10 microM Tb(3+) ions to the unfolded state of apo-ACF II, respectively, without changing the concentration of the denaturant. Using Tb(3+) as a fluorescence probe of Ca(2+), the kinetic results of metal ion-induced refolding provide evidence for the fact that the first phase of Tb(3+)-induced refolding should involve the formation of the compact metal-binding site regions, and subsequently, the protein undergoes further conformational rearrangements to form the native structure.     

Consideration of the Possibility that the slow step in protein denaturation reactions is due to cis-trans isomerism of proline residues.

A model is proposed to account for the observation that the denaturation of small proteins apparently occurs in two kinetic phases. It is suggested that only one of these phases--the fast one--is actually an unfolding process. The slow phase is assumed to arise from the cis-trans isomerism of proline residues in the denaturated protein. From model compound data, it is shown that the expected rate for isomerism is in satisfactory agreement with the rates actually observed for protein folding. It is also shown that a simple model of protein unfolding based on the isomerism concept is very successful in accounting for many known experimental characteristics of the kinetics and thermodynamic of protein denaturation. Thus, the model is able to predict that two kinetic phases will be seen in the transition region while none are seen in the base-line regions, that both the fast and slow refolding phases lead to the native protein as the product, that the fast phase becomes the only observable phase for jumps ending far in the denatured base-line region, that most or all small proteins show a limiting low-temperature activation energy of ca. 20,000 cal, and that the relaxtion time for the slow phase seen in cytochrome c denaturation is much shorter than for all other small proteins. By utilizing "double-jump" experiments, it is shown directly that the slow phase is not part of the unfolding process but that it corresponds to a transition among two or more denatured forms which have identical spectroscopic (286.5 nm) properties. Thus, the slow relaxation is "invisible" except in the transition region where it couples to the fast unfolding equilibrium. Finally, since the present model assumes that only one of the major kinetic phases seen in denaturation reactions is concerned with the denaturation process per se, it is in agreement with numerous thermodynamic studies which show consistency with the two-state model for unfolding.     

Ca(II)- and Tb(III)-induced stabilization and refolding of anticoagulation factor I from the venom of Agkistrodon acutus

Anticoagulation factor I (ACF I) isolated from the venom of Agkistrodon acutus is an activated coagulation factor X-binding protein in a Ca(2+)-dependent fashion with marked anticoagulant activity. The equilibrium unfolding/refolding of apo-ACF I, holo-ACF I, and Tb(3+)-reconstituted ACF I in guanidine hydrochloride (GdnHCl) solutions was studied by following the fluorescence and circular dichroism. Metal ions were found to increase the structural stability of ACF I against GdnHCl and thermal denaturation and, furthermore, influence its unfolding/refolding behavior. The GdnHCl-induced unfolding/refolding of both apo-ACF I and Tb(3+)-ACF I is a two-state process with no detectable intermediate state(s), whereas the GdnHCl-induced unfolding/refolding of holo-ACF I in the presence of 1 mM Ca(2+) follows a three-step transition, with intermediate state a (Ia) and intermediate state b (Ib). Ca(2+) ions play an important role in the stabilization of the Ia and Ib states. The decalcification of holo-ACF I shifts the ending zone of unfolding/refolding curve toward lower GdnHCl concentration, whereas the reconstitution of apo-ACF I with Tb(3+) ions shifts the initial zone of denaturation curve toward higher GdnHCl concentration. Therefore, it is possible to find a denaturant concentration (2.0 M GdnHCl) at which refolding from the fully denatured state of apo-ACF I to the Ib state of holo-ACF I or to the native state of Tb(3+)-ACF I can be initiated merely by adding the 1 mM Ca(2+) ions or 10 microM Tb(3+) ions to the unfolded state of apo-ACF I, respectively, without changing the concentration of the denaturant. Using Tb(3+) as a fluorescence probe of Ca(2+), the kinetic results of metal ions-induced refolding provide evidence that the compact Tb(3+)-binding region forms first, and subsequently, the protein undergoes further conformational rearrangements to form the native structure.     

Assessment study on the high-performance liquid chromatography-type hydroxyapatite chromatography in the presence of sodium dodecyl sulfate.

The HPLC-type hydroxyapatite chromatography in the presence of sodium dodecyl sulfate (SDS) was assessed with special attention to the behavior of the surfactant. A significant amount of SDS was found to be adsorbed to the hydroxyapatite packed in the column from the starting buffer, 50 mM sodium phosphate buffer, pH 7.0, only when the buffer contained SDS in a concentration at or above its critical micelle concentration. When the phosphate buffer concentration was increased while the SDS concentration was kept at 1 mg/ml, the adsorbed surfactant was desorbed in advance of the release of proteins. Polypeptides derived from proteins could be successfully separated only when the column had been thoroughly equilibrated with the above-mentioned starting buffer solution. When a protein polypeptide complexed with SDS, which had been similarly equilibrated, was applied to the column, an amount of SDS corresponding to 75-90% (w/w) of the surfactant originally bound to the polypeptide was released upon its binding to the hydroxyapatite. On the other hand, porin, an Escherichia coli outer membrane protein, retaining its trimeric native structure in the presence of SDS, released a significantly smaller amount of SDS. When the membrane protein was denatured to give a single polypeptide, it behaved in a manner similar to that of the other protein polypeptides. The mechanism of binding of the protein polypeptides was discussed on the basis of these results. The native and denatured entities of porin could be efficiently separated as the result of the difference in their mode of interaction with the hydroxyapatite.     

Water and urea interactions with the native and unfolded forms of a beta-barrel protein

A fundamental understanding of protein stability and the mechanism of denaturant action must ultimately rest on detailed knowledge about the structure, solvation, and energetics of the denatured state. Here, we use (17)O and (2)H magnetic relaxation dispersion (MRD) to study urea-induced denaturation of intestinal fatty acid-binding protein (I-FABP). MRD is among the few methods that can provide molecular-level information about protein solvation in native as well as denatured states, and it is used here to simultaneously monitor the interactions of urea and water with the unfolding protein. Whereas CD shows an apparently two-state transition, MRD reveals a more complex process involving at least two intermediates. At least one water molecule binds persistently (with residence time >10 nsec) to the protein even in 7.5 M urea, where the large internal binding cavity is disrupted and CD indicates a fully denatured protein. This may be the water molecule buried near the small hydrophobic folding core at the D-E turn in the native protein. The MRD data also provide insights about transient (residence time <1 nsec) interactions of urea and water with the native and denatured protein. In the denatured state, both water and urea rotation is much more retarded than for a fully solvated polypeptide. The MRD results support a picture of the denatured state where solvent penetrates relatively compact clusters of polypeptide segments.     

The cold denatured state is compact but expands at low temperatures: hydrodynamic properties of the cold denatured state of the C-terminal domain of L9

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

Denaturant-gradient chromatography for the study of protein denaturation: principle and procedure

The particle volume of a protein which represents the expansion of the molecular chain is a useful probe to measure its conformation change in solution. To study the details of the conformation transition, we will report a novel device to trace the particle-volume change against increasing denaturant concentration. According to the denaturant gradient in the eluant of high-performance gel-permeation chromatography, information concerning the elution volume of proteins in the course of denaturation can be successively accessed. When a protein is injected into a denaturant solution, its effective molecular volume increases by the unfolding of a native compact structure, and the elution peak goes forward to separate from that of the native protein. Typical elution patterns were computer-simulated in an extended algorithm of the plate theory. The kinetic feature of denaturation and the effect of the denaturant gradient are discussed. The denaturation schemes of lysozyme, cytochrome c, and phosphoglycerate kinase were studied.     

Denatured states of ribonuclease A have compact dimensions and residual secondary structure.

Using small-angle X-ray scattering and Fourier transform infrared spectroscopy, we have determined that the thermally denatured state of native ribonuclease A is on average a compact structure having residual secondary structure. Under strongly reducing conditions, the protein further unfolds into a looser structure with larger dimensions but still retains a comparable amount of secondary structure. The dimensions of the thermally and chemically denatured states of the reduced protein are different but both are more compact than is predicted for a random coil of the same length. These results demonstrate that thermal denaturation in ribonuclease A is not a simple two-state transition from a native to a completely disordered random coil state.