Thermodynamic analysis of denaturant-induced unfolding of HodC69S protein supports a three-state mechanism.

Thermodynamic stability parameters and the equilibrium unfolding mechanism of His 6HodC69S, a mutant of 1 H-3-hydroxy-4-oxoquinaldine 2,4-dioxygenase (Hod) having a Cys to Ser exchange at position 69 and an N-terminal hexahistidine tag (His 6HodC69S), have been derived from isothermal unfolding studies using guanidine hydrochloride (GdnHCl) or urea as denaturants. The conformational changes were monitored by following changes in circular dichroism (CD), fluorescence, and dynamic light scattering (DLS), and the resulting transition curves were analyzed on the basis of a sequential three-state model N = I = D. The structural changes have been correlated to catalytic activity, and the contribution to stability of the disulfide bond between residues C37 and C184 in the native protein has been established. A prominent result of the present study is the finding that, independent of the method used for denaturing the protein, the unfolding mechanism always comprises three states which can be characterized by, within error limits, identical sets of thermodynamic parameters. Apparent deviations from three-state unfolding can be rationalized by the inability of a spectroscopic probe to discriminate clearly between native, intermediate, and unfolded ensembles. This was the case for the CD-monitored urea unfolding curve.

Stability, unfolding, and structural changes of cofactor-free 1H-3-hydroxy-4-oxoquinaldine 2,4-dioxygenase.

Stability, unfolding mechanism, spectroscopic, densimetric, and structural characteristics of the oxidatively stable C69S variant (HodC) of 1H-3-hydroxy-4-oxoquinaldine 2,4-dioxygenase (Hod) have been determined by classical and pressure modulation scanning calorimetry (DSC and PMDSC, respectively), circular dichroism (CD) spectroscopy, differential scanning densimetry (DSD), and dynamic light scattering measurements. At 25 degrees C, hexahistidine-tagged HodC has a hydrodynamic radius of 2.3 nm and is characterized by an unusually high degree of alpha-helical structure of approximately 60%, based on deconvolution of CD spectra. The percentage of beta-sheets and -turns is expected to be relatively low in view of its sequence similarity to proteins of the alpha/beta-hydrolase fold superfamily. His6HodC exhibits three-state unfolding (N <--> I <--> D) with an intermediate state I that exhibits at the transition temperature a volume larger than that of the native or denatured state. The intermediate state I is also associated with the highest isothermal expansion coefficient, alphaP, of the three states and exhibits a significantly lower percentage of alpha-helical structure than the native state. The stability difference between the native and intermediate state is rather small which makes I a potential candidate for reactions with various ligands, particularly those having a preference for the apparently preserved beta-type motifs.

Pressure-modulated differential scanning calorimetry. An approach to the continuous, simultaneous determination of heat capacities and expansion coefficients.

A new method is described that permits the continuous and synchronous determination of heat capacity and expansibility data. We refer to it as pressure-modulated differential scanning calorimetry (PMDSC), as it involves a standard DSC temperature scan and superimposes on it a pressure modulation of preselected format. The power of the method is demonstrated using salt solutions for which the most accurate heat capacity and expansibility data exist in the literature. As the PMDSC measurements could reproduce the parameters with high accuracy and precision, we applied the method also to an aqueous suspension of multilamellar DSPC vesicles for which no expansibility data had been reported previously for the transition region. Excellent agreement was obtained between data from PMDSC and values from independent direct differential scanning densimetry measurements. The basic theoretical background of the method when using sawtooth-like pressure ramps is given under Supporting Information, and a complete statistical thermodynamic derivation of the general equations is presented in the accompanying paper.

Matrix-assisted in vitro refolding of Pseudomonas aeruginosa class II polyhydroxyalkanoate synthase from inclusion bodies produced in recombinant Escherichia coli.

In order to facilitate the large-scale preparation of active class II polyhydroxyalkanoate (PHA) synthase, we constructed a vector pT7-7 derivative that contains a modified phaC1 gene encoding a PHA synthase from Pseudomonas aeruginosa possessing six N-terminally fused histidine residues. Overexpression of this phaC1 gene under control of the strong Ø10 promoter was achieved in Escherichia coli BL21(DE3). The fusion protein was deposited as inactive inclusion bodies in recombinant E. coli, and contributed approx. 30% of total protein. The inclusion bodies were purified by selective solubilization, resulting in approx. 70-80% pure PHA synthase, then dissolved and denatured by 6 M guanidine hydrochloride. The denatured PHA synthase was reversibly immobilized on a Ni(2+)-nitrilotriacetate-agarose matrix. The matrix-bound fusion protein was refolded by gradual removal of the chaotropic reagent. This procedure avoided the aggregation of folding intermediates which often decreases the efficiency of refolding experiments. Finally, the refolded fusion protein was eluted with imidazole. The purified and refolded PHA synthase protein showed a specific enzyme activity of 10.8 m-units/mg employing (R/S)-3-hydroxydecanoyl-CoA as substrate, which corresponds to 27% of the maximum specific activity of the native enzyme. The refolding of the enzyme was confirmed by CD spectroscopy. Deconvolution of the spectrum resulted in the following secondary structure prediction: 10% alpha-helix, 50% beta-sheet and 40% random coil. Gel filtration chromatography indicated an apparent molecular mass of 69 kDa for the refolded PHA synthase. However, light-scattering analysis of a 10-fold concentrated sample indicated a molecular mass of 128 kDa. These data suggest that the class II PHA synthase is present in an equilibrium of monomer and dimer.

Folding energetics of ligand binding proteins. I. Theoretical model.

Heat capacity curves as obtained from differential scanning calorimetry are an outstanding source for molecular information on protein folding and ligand-binding energetics. However, deconvolution of C(p) data of proteins in the presence of ligands can be compromised by indeterminacies concerning the correct choice of the statistical thermodynamic ensemble. By convent, the assumption of constant free ligand concentration has been used to derive formulae for the enthalpy. Unless the ligand occurs at large excess, this assumption is incorrect. Still the relevant ensemble is the grand canonical ensemble. We derive formulae for both constraints, constancy of total or free ligand concentration and illustrate the equations by application to the typical equilibrium Nx <=> N + x <=> D + x. It is demonstrated that as long as the thermodynamic properties of the ligand can be completely corrected for by performing a reference measurement, the grand canonical approach provides the proper and mathematically significantly simpler choice. We demonstrate on the two cases of sequential or independent ligand-binding the fact, that similar binding mechanisms result in different and distinguishable heat capacity equations. Finally, we propose adequate strategies for DSC experiments as well as for obtaining first estimates of the characteristic thermodynamic parameters, which can be used as starting values in a global fit of DSC data.

Folding energetics of ligand binding proteins II. Cooperative binding of Ca2+ to annexin I.

The calcium binding properties of annexin I as observed by thermodynamic DSC studies have been compared to the structural information obtained from X-ray investigation. The calorimetric experiment permitted to evaluate both the reaction scheme - including binding of ligand and conformational changes - and the energetics of each reaction step. According to published X-ray data Annexin I has six calcium binding sites, three medium-affinity type II and three low-affinity type III sites. The present study shows that at 37 degrees C annexin I binds in a Hill type fashion simultaneously two calcium ions in a first step with medium affinity at a concentration of 0.6 mM and another three Ca(2+) ions again cooperatively at 30 mM with low affinity. Therefore it can be concluded that only two medium-affinity type II binding sites are available. The third site, that should be accessible in principle appears to be masked presumably due to the presence of the N terminus. In view of the large calcium concentration needed for saturation of the binding sites, annexin I may be expected to be Ca(2+) free in vivo unless other processes such as membrane interaction occur simultaneously. This assumption is consistent with the finding, that the affinity of annexins to calcium is usually markedly increased by the presence of lipids.

alpha 2beta 1 integrin is not recognized by rhodocytin but is the specific, high affinity target of rhodocetin, an RGD-independent disintegrin and potent inhibitor of cell adhesion to collagen.

We have recombinantly expressed a soluble form of human alpha(2)beta(1) integrin that lacks the membrane-anchoring transmembrane domains as well as the cytoplasmic tails of both integrin subunits. This soluble alpha(2)beta(1) integrin binds to its collagen ligands the same way as the wild-type alpha(2)beta(1) integrin. Furthermore, like the wild-type form, it can be activated by manganese ions and an integrin-activating antibody. However, it does not bind to rhodocytin, a postulated agonist of alpha(2)beta(1) integrin from the snake venom of Calloselasma rhodostoma, which elicits platelet aggregation. Taking advantage of the recombinantly expressed, soluble alpha(2)beta(1) integrin, an inhibition assay was established in which samples can be tested for their capability to inhibit binding of soluble alpha(2)beta(1) integrin to immobilized collagen. Thus, by scrutinizing the C. rhodostoma snake venom in this protein-protein interaction assay, we found a component of the snake venom that inhibits the interaction of soluble alpha(2)beta(1) integrin to type I collagen efficiently. N-terminal sequences identified this inhibitor as rhodocetin, a recently published antagonist of collagen-induced platelet aggregation. We could demonstrate that its inhibitory effect bases on its strong and specific binding to alpha(2)beta(1) integrin, proving that rhodocetin is a disintegrin. Standing apart from the growing group of RGD-dependent snake venom disintegrins, rhodocetin interacts with alpha(2)beta(1) integrin in an RGD-independent manner. Furthermore, its native conformation, which is stabilized by disulfide bridges, is indispensibly required for its inhibitory activity. Rhodocetin does not contain any major collagenous structure despite its high affinity to alpha(2)beta(1) integrin, which binds to collagenous molecules much more avidly than to noncollagenous ligands, such as laminin. Blocking alpha(2)beta(1) integrin as the major collagen receptor on platelets, rhodocetin is responsible for hampering collagen-induced, alpha(2)beta(1) integrin-mediated platelet activation, leading to hemorrhages and bleeding disorders of the snakebite victim. Moreover, having a widespread tissue distribution, alpha(2)beta(1) integrin also mediates cell adhesion, spreading, and migration. We showed that rhodocetin is able to inhibit alpha(2)beta(1) integrin-mediated adhesion of fibrosarcoma cells to type I collagen completely.

Protein heat capacity reflects the dynamics of enthalpy exchange between the single macromolecule and the surroundings.

Heat capacity has played a prominent role in relating macroscopic and microscopic properties of small molecules and crystals. However, its diagnostic power can also be used for macromolecules such as proteins. It is shown in the present study that the macroscopically observed protein heat capacity provides direct access to the thermodynamic state of the single protein molecule. The new model of the physical basis of protein heat capacity emphasizes the dynamic nature of protein molecules. It incorporates equilibrium fluctuations as an integral constituent and shows that the increase in the magnitude of equilibrium fluctuations is coupled to an increase in the enthalpy flux between the individual protein molecule and its surroundings.

Response functions of proteins.

The thermodynamics of protein folding can be studied by a variety of different techniques such as differential scanning calorimetry, differential scanning densimetry and sound velocity measurements. These three methods monitor the different response functions heat capacity, expansion coefficient and compressibility that characterise various aspects of protein dynamics such as equilibrium energy and volume fluctuations and energy-volume correlations. For the development of a comprehensive thermodynamic description of protein behaviour information on these response functions should be combined. As a starting point we provide in the present paper analytical solutions for the determination of the response functions and demonstrate on several examples how to extract a maximum of thermodynamic information on proteins from the measurements of Cp, alpha p and kappa T.

Slow unfolding and refolding kinetics of the mesophilic Rop wild-type protein in the transition range.

We describe the guanidinium hydrochloride induced folding kinetics of the four-helix-bundle protein Rop wild-type (wt) under equilibrium conditions at three temperatures. The choice of appropriate denaturant conditions inside the transition range permitted, in combination with equilibrium transition curves, the determination of both unfolding and refolding rate constants. The ratio of the rate constants at zero denaturant concentration provided equilibrium constants and standard free energy changes that are in good agreement with values obtained in previous differential scanning calorimetry studies. The DeltaG0D values for 19, 25 and 40 degrees C calculated from the present kinetic studies are, respectively, 66.8, 70.8 and 57.2 kJ.mol-1. The unfolding reactions are extremely slow under these conditions. Equilibrium was reached only after 18, 12 and 6 days at 19, 25 and 40 degrees C. These results demonstrate that for Rop wt high stability correlates with slow folding kinetics.

A new set of peptide-based group heat capacities for use in protein stability calculations.

The partial molar heat capacities of the tripeptides of the sequence glycyl-X-glycine, where X is one of the amino acids leucine, threonine, glutamine, phenylalanine, histidine, cysteine, proline, glutamic acid or arginine, and of the two tetrapeptides tetraglycine and glycyltryptophanylglycylglycine in aqueous solution over the temperature range 10-100 degrees C have been determined using high sensitivity scanning microcalorimetry. These results were used to derive the partial molar heat capacities of the various amino acid side-chains. This report completes our programme to derive reliable side-chain heat capacities for all 20 amino acids of proteins over a wide temperature range using the tripeptides Gly-X-Gly as realistic model compounds. Included in the study is a summary of the partial molar heat capacities of all 20 amino acid side-chains. These results, along with the heat capacity of the peptide backbone group, were used to calculate the partial molar heat capacities of some oligopeptides and of the random coil form of some unfolded proteins in water. The calculated heat capacities of the proteins obtained using this new set of heat capacities for the constituent groups are consistent with the heat capacities of the denatured state determined experimentally.

Stability and binding properties of wild-type and c17s mutated human sterol carrier protein 2.

The temperature- and solvent-induced denaturation of both the SCP2 wild-type and the mutated protein c71s were studied by CD measurements at 222 nm. The temperature-induced transition curves were deconvoluted according to a two-state mechanism resulting in a transition temperature of 70.5 degrees C and 59.9 degrees C for the wild-type and the c71s, respectively, with corresponding values of the van't Hoff enthalpies of 183 and 164 kJ/mol. Stability parameters characterizing the guanidine hydrochloride denaturation curves were also calculated on the basis of a two-state transition. The transitions of the wild-type occurs at 0.82 M GdnHCl and that of the c71s mutant at 0.55 M GdnHCl. These differences in the half denaturation concentration of GdnHCl reflect already the significant stability differences between the two proteins. A quantitative measure are the Gibbs energies DeltaG(0)(D)(buffer) at 25 degrees C of 15.5 kJ/mol for the wild-type and 8.0 kJ/mol for the mutant. We characterized also the alkyl chain binding properties of the two proteins by measuring the interaction parameters for the complex formation with 1-O-Decanyl-beta-D-glucoside using isothermal titration microcalorimetry. The dissociation constants, K(d), for wild-type SCP2 are 335 microM at 25 degrees C and 1.3 mM at 35 degrees C. The corresponding binding enthalpies, DeltaH(b), are -21. 5 kJ/mol at 25 degrees C and 72.2 kJ/mol at 35 degrees C. The parameters for the c71s mutant at 25 degrees C are K(d)=413 microM and DeltaH(b)=16.6 kJ/mol. These results suggest that both SCP2 wild-type and the c71s mutant bind the hydrophobic compound with moderate affinity.

Refolding studies on the tetrameric loop deletion mutant RM6 of ROP protein.

Previous DSC and X-ray studies on RM6, a loop deletion mutant of wtROP protein, have shown that removal of five amino acids from the loop causes a dramatic reorganization of the wild-type structure. The new tetrameric molecule exhibits a significantly higher stability (Lassalle, M.W. et al., J. Mol. Biol., 1998, 279, 987-1000) and unfolds in a second order reaction (Lassalle, M.W. and Hinz, H.-J., Biochemistry, 1998, 37, 8465-8472). In the present investigation we report extensive refolding studies of RM6 at different temperatures and GdnHCl concentrations monitored by CD and fluorescence to probe for changes in secondary and tertiary structure, respectively. The measurements permitted us to determine activation parameters as a function of denaturant concentration. The results demonstrate convincingly that the variation with GdnHCl concentration of the activation parameters deltaH#, deltaS# and deltaG# is very similar for unfolding and refolding. For both processes the activation properties approach a maximum in the vicinity of the denaturant concentration, c(K=1), where the equilibrium constant equals 1, i.e. deltaG0 equals zero. CD and fluorescence refolding kinetics are described by identical constants suggesting that the formation of secondary and tertiary structure occurs simultaneously. Refolding is, however, characterized by a more complex mechanism than unfolding. Although the general pattern is dominated by the sequence monomers to dimers to tetramers, parallel side reactions involving dimers and monomers have to be envisaged in the initial folding phase, supporting the view that the native state of RM6 can be reached by several rather than a single pathway.

A comparison of the energetics of annexin I and annexin V.

The annexins comprise a family of soluble Ca2+- and phospholipid-binding proteins. Although highly similar in three-dimensional structure, different annexins are likely to exhibit different biochemical and functional properties and to play different roles in various membrane related events. Since it must be expected that these functional differences arise from differences in the characteristic thermodynamic parameters of these proteins, we performed high-sensitivity differential scanning microcalorimetry (DSC) and isothermal guanidinium hydrochloride (GdnHCl)-induced unfolding studies on annexin I and compared its thermodynamic parameters with those of annexin V published previously. The DSC data were analyzed using a model that permits quantitative treatment of the irreversible reaction. It turned out, however, that provided a heating rate of 2 K min-1 is used, unfolding of annexin I can be described satisfactorily in terms of a simple two-state reaction. At pH 6.0 annexin I is characterized by the following thermodynamic parameters: t1/2=61.8 degrees C, DeltaHcal=824 kJ mol-1 and DeltaCp=19 kJ mol-1 K-1. These parameters result in a stability value of DeltaG0D (20 degrees C)=51 kJ mol-1. The GdnHCl induced isothermal unfolding of annexin I in Mes buffer (pH 6.0), yielded DeltaG0D (buffer) values of 48, 60 and 36 kJ mol-1 at 20, 12 and 5 degrees C, respectively. These DeltaG0D values are in reasonable agreement with the values obtained from the DSC studies. The comparison of annexin I and annexin V under identical conditions (pH 8.0 or pH 6.0) shows that despite the pronounced structural homology of these two members of the annexin familiy, the stability parameters are remarkably different. This difference in stability is consistent with and provides a thermodynamic basis for the potential different in vivo functions proposed for these two annexins.

Protein heat capacity: inconsistencies in the current view of cold denaturation.

The present study shows on the basis of the thermodynamic stability criterion (partial differential S/partial differential T)p>0 that partitioning of the entropy of cold-unfolding of a protein into independent positive conformational and negative hydrational contributions is incorrect. Furthermore it provides a new microscopic interpretation of protein heat capacity that takes into account the significant fluctuations in energy and entropy which result from the small size of these macromolecules.

Partial molar volumes of proteins: amino acid side-chain contributions derived from the partial molar volumes of some tripeptides over the temperature range 10-90 degrees C.

The partial molar volumes of tripeptides of sequence glycyl-X-glycine, where X is one of the amino acids alanine, leucine, threonine, glutamine, phenylalanine, histidine, cysteine, proline, glutamic acid, and arginine, have been determined in aqueous solution over the temperature range 10-90 degrees C using differential scanning densitometry . These data, together with those reported previously, have been used to derive the partial molar volumes of the side-chains of all 20 amino acids. The side-chain volumes are critically compared with literature values derived using partial molar volumes for alternative model compounds. The new amino acid side-chain volumes, along with that for the backbone glycyl group, were used to calculate the partial specific volumes of several proteins in aqueous solution. The results obtained are compared with those observed experimentally. The new side-chain volumes have also been used to re-determine residue volume changes upon protein folding.

Ca2+-independent interaction of annexin I with phospholipid monolayers.

At pH 6.0, the interaction of annexin I, a proteolytic fragment of annexin I and annexin V, was studied with monolayers composed of dipalmitoylphosphatidylserine (DPPS), dipalmitoylphosphatidylcholine (DPPC) or DPPS/DPPC mixtures (molar ratio 1:4). The measurements reveal that only annexin I shows a significant increase in the surface pressure at constant surface area in the absence of Ca2+ ions. We interpret these pressure changes as reflecting penetration of the protein. Kinetic analyses of the annexin I/monolayer interaction at pH 6.0 in the presence and absence of Ca2+ ions show differences between the interaction mechanisms that support the occurrence of a pH-regulated process. At pH 7.4, Ca2+ ions are required for the interaction.

Dimer-to-tetramer transformation: loop excision dramatically alters structure and stability of the ROP four alpha-helix bundle protein.

The ROP loop excision mutant RM6 shows dramatic changes in structure and stability in comparison to the wild-type protein. Removal of the five amino acids (Asp30, Ala31, Asp32, Glu33, Gln34) from the loop results in a complete reorganization of the protein as evidenced by single crystal X-ray analysis and thermodynamic unfolding studies. The homodimeric four-alpha-helix motif of the wild-type structure is given up. Instead a homotetrameric four-alpha-helix structure with extended, loop-free helical monomers is formed. This intriguing structural change is associated with the acquisition of hyperthermophilic stability. This is evident in the shift in transition temperature from 71 degreesC characteristic of the wild-type protein to 101 degreesC for RM6. Accordingly the Gibbs energy of unfolding is increased from 71.7 kJ (mol of dimer)-1 to 195.1 kJ (mol of tetramer)-1. The tetramer-to-monomer transition proceeds highly cooperatively involving an enthalpy change of DeltaH=1073+/-30 kJ (mol of tetramer)-1 and a heat capacity change at the transition temperature of DeltaDNCp=14.9(+/-)3% kJ (mol of tetramerxK)-1. The two-state nature of the unfolding reaction is reflected in coinciding calorimetric and van't Hoff enthalpy values.

Unfolding of the tetrameric loop deletion mutant of ROP protein is a second-order reaction.

Comprehensive kinetic studies were carried out on the unfolding properties of RM6 as a function of GdnHCl concentration and temperature. This protein is a mutant resulting from the dimeric wild-type CoLE1-ROP protein by deletion of 5 amino acids (Asp 30, Ala 31, Asp 32, Glu 33, Gln 34) in the loop of each monomer. The deletion has dramatic consequences. The dimeric 4-alpha-helix structure characteristic of the wild-type protein is completely reorganized and the RM6 structure can be described as a tetrameric alpha helix of extended monomers without loops. These extraordinary structural changes are accompanied by an enormous increase in transition temperature from 71 to 101 degreesC. These features have been discussed in a separate publication (1). The remarkable change in thermal stability of RM6 should be reflected in significant changes in the folding rate constants. This was observed in the present unfolding studies. Decay of tetrameric RM6 was monitored by circular dichroism (CD) and fluorescence to probe for changes in both secondary and tertiary structure, respectively. The identity of the kinetic parameters obtained from the two techniques supports the view that secondary and tertiary structure break down simultaneously. However, the most intriguing result is the finding that unfolding of tetrameric RM6 can be described very well by a second-order reaction. The magnitude of the second-order rate constant k2 varies dramatically with both temperature and denaturant concentration. At 25 degreesC and 6.5 M GdnHCl concentration k2 is 4200 L.(mol of dimer)-1.s-1, whereas at 4.4 M GdnHCl a value of k2 = 0.9 L.(mol of dimer)-1.s-1 is observed. Correspondingly, apparent activation enthalpies show a strong increase from DeltaH# = 29.1 kJ.mol-1 at 6. 5 M GdnHCl to Delta H# = 79.7 kJ.mol-1 at 4.4 M GdnHCl. A mechanism involving a dimeric intermediate is suggested which permits a consistent interpretation of the findings.

Acid induced equilibrium unfolding of annexin V wild type shows two intermediate states.

Annexin V is an alpha-helical protein which shows anticoagulatory and antiinflammatory activity. It is supposed to be involved in membrane fusion and exocytosis. In this study acid-induced equilibrium unfolding of the human annexin V is investigated by fluorescence and circular dichroism spectroscopy. The spectroscopic data indicate that at least two intermediate states are involved in unfolding. One of the proposed intermediate states exhibits properties similar to those observed with annexin V wild type saturated with calcium, another may be regarded as 'molten globule'.