Microcalorimetric study of the heat denaturation of carboanhydrase B

The microcalorimetric study of heat denaturation of carbonic anhydrase B has revealed that the process of denaturation of carbonic anhydrase B is accompanied by the formation of intermolecular complexes which are disrupted at a further increase of temperature. It is shown that zinc atoms stabilize the native state and do not influence the stability of intermolecular complexes.     

Thermal conformational transformations of tropocollagen. II. Viscometric and light-scattering studies

It was shown by viscometric measurements that a tropocollagen solution at low shear gradients manifests elastic features which can be connected only with the existence of a labile spatial structure which develops in time in the solution. To judge by the concentration dependence of the rate of formation of this structure, it does not represent a molecular net formed by direct contact of macromolecules. Most likely this structure is a result of stabilization of macromolecules at a certain distance from each other. The study of light scattering by tropocollagen solutions demonstrated that it does not correspond with the scattering by rigid rod-shaped units. Anomalies in the character of light scattering are probably the result of intermolecular interference produced by a spatial supermolecular structure and, in turn, indicate that this structure is to some extent regular. In the presence of salts the elastic features in the tropocollagen solution and anomalies in light scattering disappear in a narrow range of temperatures immediately before the process of denaturation which makes it possible to conclude that the supermolecular regular structure is disrupted in this temperature range.     

Calorimetric study of the heat and cold denaturation of beta-lactoglobulin.

Temperature-induced changes of the states of beta-lactoglobulin have been studied calorimetrically. In the presence of a high concentration of urea this protein shows not only heat but also cold denaturation. Its heat denaturation is approximated very closely by a two-state transition, while the cold denaturation deviates considerably from the two-state transition and this deviation increases as the temperature decreases. The heat effect of cold denaturation is opposite in sign to that of heat denaturation and is noticeably larger in magnitude. This difference in magnitude is caused by the temperature-dependent negative heat effect of additional binding of urea to the polypeptide chain of the protein upon its unfolding, which decreases the positive enthalpy of heat denaturation and increases the negative enthalpy of cold denaturation. The binding of urea considerably increases the partial heat capacity of the protein, especially in the denatured state. However, when corrected for the heat capacity effect of urea binding, the partial heat capacity of the denatured protein is close in magnitude to that expected for the unfolded polypeptide chain in aqueous solution without urea but only for temperatures below 10 degrees C. At higher temperatures, the heat capacity of the denatured protein is lower than that expected for the unfolded polypeptide chain. It appears that at temperatures above 10 degrees C not all the surface of the beta-lactoglobulin polypeptide chain is exposed to the solvent, even in the presence of 6 M urea; i.e., the denatured protein is not completely unfolded and unfolds only at temperatures lower than 10 degrees C.(ABSTRACT TRUNCATED AT 250 WORDS)     

Thermodynamics of staphylococcal nuclease denaturation. II. The A-state.

Staphylococcal nuclease, at low pH and in the presence of high salt concentrations, has previously been proposed to exist in a partially folded or molten globule form called the "A-state" (Fink et al., 1993, Protein Sci 2:1155-1160). We have found that the A-state of nuclease at pH 2.1 in the presence of moderate to high salt concentrations and at low temperature exists in a substantially folded form structurally more similar to a native state. The A-state has the far-UV circular dichroism spectra characteristic of the native protein, which indicates that it has a large degree of secondary structure. Upon heating, the A-state denatures with a sigmoidal change in far-UV ellipticity and an observable peak in a differential scanning calorimeter trace, indicating that it is thermodynamically distinct from the denatured state. Three different mutations in a residue normally buried in the protein's core stabilize or destabilize the A-state in the same way as they affect the denaturation of the native state. The A-state must, therefore, contain at least some tertiary packing of side chains. Unlike the native state, which shows cold denaturation at low temperatures, the A-state is most stable at temperatures below 0 degrees C.     

Thermodynamics of ubiquitin unfolding

The energetics of ubiquitin unfolding have been studied using differential scanning microcalorimetry. For the first time it has been shown directly that the enthalpy of protein unfolding is a nonlinear function of temperature. Thermodynamic parameters of ubiquitin unfolding were correlated with the structure of the protein. The enthalpy of hydrogen bonding in ubiquitin was calculated and compared to that obtained for other proteins. It appears that the energy of hydrogen bonding correlates with the average length of the hydrogen bond in a given protein structure. © 1994 John Wiley & Sons, Inc.     

Structural energetics of barstar studied by differential scanning microcalorimetry.

The energetics of barstar denaturation have been studied by CD and scanning microcalorimetry in an extended range of pH and salt concentration. It was shown that, upon increasing temperature, barstar undergoes a transition to the denatured state that is well approximated by a two-state transition in solutions of high ionic strength. This transition is accompanied by significant heat absorption and an increase in heat capacity. The denaturational heat capacity increment at approximately 75 degrees C was found to be 5.6 +/- 0.3 kJ K-1 mol-1. In all cases, the value of the measured enthalpy of denaturation was notably lower than those observed for other small globular proteins. In order to explain this observation, the relative contributions of hydration and the disruption of internal interactions to the total enthalpy and entropy of unfolding were calculated. The enthalpy and entropy of hydration were found to be in good agreement with those calculated for other proteins, but the enthalpy and entropy of breaking internal interactions were found to be among the lowest for all globular proteins that have been studied. Additionally, the partial specific heat capacity of barstar in the native state was found to be 0.37 +/- 0.03 cal K-1 g-1, which is higher than what is observed for most globular proteins and suggests significant flexibility in the native state. It is known from structural data that barstar undergoes a conformational change upon binding to its natural substrate barnase.(ABSTRACT TRUNCATED AT 250 WORDS)     

Contribution of hydration and non-covalent interactions to the heat capacity effect on protein unfolding.

The heat capacity change upon protein unfolding has been analysed using the heat capacity data for the model compounds' transfer into water, corrected for volume effects. It has been shown that in the unfolding, the heat capacity increment is contributed to by the effect of hydration of the non-polar groups, which is positive and decreases with temperature increase, and by the effect of hydration of the polar groups, which is negative and decreases in magnitude as temperature increases. The sum of these two effects is very close to the total heat capacity increment of protein unfolding at room temperature but is likely to deviate from it at higher temperatures. Therefore, the expected heat capacity effect caused by the increase of configurational freedom of the polypeptide chain upon unfolding seems to be compensated for by some other effect, perhaps associated with fluctuation of the native protein structure.     

Calorimetric study of tryptophan synthase alpha-subunit and two mutant proteins

Heat-denaturation of tryptophan synthase alpha-subunit from E. coli and two mutant proteins (Glu 49 leads to Gln or Ser; called Gln 49 or Ser 49, respectively) has been studied by the scanning microcalorimetric method at various pH, in an attempt to elucidate the role of individual amino acid residues in the conformational stability of a protein. The partial specific heat capacity in the native state at 20 degrees, Cp20, has been found to be (0.43 +/- 0.02) cal . k-1 . g-1, the unfolding heat capacity change, delta dCp, (0.10 +/- 0.01) cal . K-1 . g-1, and the unfolding enthalpy value extrapolated to 110 degrees, delta dh110, (9.3 +/- 0.5) cal . g-1 for the three proteins. The value of Cp20 was larger than those found for "fully compact protein" and that of delta dh110 was smaller. Unfolding Gibbs energy, delta dG at 25 degrees for Wild-type, Gln 49, and Ser 49 were 5.8, 8.4, and 7.1 kcal . mol-1 at pH 9.3, respectively. Unfolding enthalpy, delta dH, of the three proteins seemed to be the same and equal to (23.2 +/- 1.2) kcal . mol-1 at 25 degrees. As a consequence of the same value of delta dH and the different value in delta dG, substantial differences in unfolding entropy, delta dS, were found for the three proteins. The values of delta dG for the three proteins at 25 degrees coincided with those from equilibrium methods of denaturation by guanidine hydrochloride.     

Heat denaturation of alpha-tropomyosin and its fragments

The reasons for three heterogeneity of tropomyosin melting curves are considered. It is shown that this phenomenon is due to the molecular heterogeneity of the preparation. Different states of the SH-groups as well as the different stability of molecule regions. The melting curves of alpha-tropomyosin and two of its fragments are obtained. The thermodynamic parameters stabilizing their helical structure are determined. The existence of a thermodynamical transition at 31 degrees C is shown for alpha-tropomyosin leading to the loss of the ability of the molecule to form supra-molecular structures.