Prothymosin is an acidic protein with an unusual amino acid composition. Though its exact function is not yet known, its high evolutionary conservation and wide tissue distribution suggest an essential biological role. Its physical state, which is controversially discussed in previous publications, was investigated using small-angle X-ray scattering, dynamic light scattering, mass spectrometry, and circular dichroism (CD). Our results unequivocally demonstrate that prothymosin is a monomer under physiological conditions. The protein adopts a random coillike conformation but exhibits persistence of direction and curvature. No regular secondary structure is detectable by CD. The Stokes radius, Rs = 3.07 nm, and the radius of gyration, RG = 4.76 nm, are 1.77 and 3.42 times larger, respectively, than those expected for a compactly folded protein consisting of 109 amino acid residues. A remarkable amount of secondary structure is formed only in the presence of trifluoroethanol at low pH. The finding that a biologically active protein molecule with 109 amino acid residues adopts a random coil conformation under physiological conditions raises the question whether this is a rare or a hitherto-overlooked but widespread phenomenon in the field of macromolecular polypeptides.

We have investigated the conformational transition and aggregation process of recombinant Syrian hamster prion protein (SHaPrP 90 -232 ) by Fourier transform infrared spectroscopy, circular dichroism spectroscopy, light scattering, and electron microscopy under equilibrium and kinetic conditions. SHaPrP 90 -232 showed an infrared absorbance spectrum typical of proteins with a predominant ␣-helical structure both at pH 7.0 and at pH 4.2 in the absence of guanidine hydrochloride. At pH 4.2 and destabilizing conditions (0.3-2 M guanidine hydrochloride), the secondary structure of SHaPrP 90 -232 was transformed to a strongly hydrogen-bonded, most probably intermolecularly arranged antiparallel ␤-sheet structure as indicated by dominant amide I band components at 1620 and 1691 cm ؊1 . Kinetic analysis of the transition process showed that the decrease in ␣-helical structures and the increase in ␤-sheet structures occurred concomitantly according to a bimolecular reaction. However, the concentration dependence of the corresponding rate constant pointed to an apparent third order reaction. No ␤-sheet structure was formed within the dead time (190 ms) of the infrared experiments. Light scattering measurements revealed that the structural transition of SHaPrP 90 -232 was accompanied by formation of oligomers, whose size was linearly dependent on protein concentration. Extrapolation to zero protein concentration yielded octamers as the smallest oligomers, which are considered as "critical oligomers." The small oligomers showed spherical and annular shapes in electron micrographs. Critical oligomers seem to play a key role during the transition and aggregation process of SHaPrP 90 -232 . A new model for the structural transition and aggregation process of the prion protein is described.The prion protein (PrP) 1 is, following the protein-only hypothesis, the sole agent causing a group of neurodegenerative disorders (1, 2), the so-called prion diseases or prionoses (3). The most important ones among them are bovine spongiform encephalopathy (BSE) in cattle, scrapie in sheep, and Creutzfeldt-Jakob disease in humans.The crucial step in transmission and manifestation of prion diseases is the conversion of benign monomeric cellular prion protein (PrP C ), which has a mainly ␣-helical secondary structure, to pathogenic multimeric scrapie prion protein (PrP Sc ), which is predominantly folded into ␤-sheets (4, 5). It is noteworthy that PrP C and PrP Sc do not differ in their amino acid sequence.Similar mechanisms play an essential role in a number of other neurodegenerative disorders including Alzheimer's, Parkinson's, and Huntington's diseases. Therefore, the coupled processes of protein misfolding and aggregation, the kinetics of these processes, and the molecular species involved are of fundamental interest.Late products of the conversion are amyloid fibrils and amyloid plaques, which are widely considered to be direct effectors of the above mentioned disorders. However, evidence is accumulating that intermediates or by-product...

Apomyoglobin undergoes a two-step unfolding transition when the pH is lowered from 6 to 2. The partly folded intermediate (I) state at pH 4 and low ionic strength has properties of a molten globule. We have studied structural features of this state, its compactness, content of secondary structure, and specific packing of aromatic side chains, using dynamic light scattering, and small-angle X-ray scattering and far- and near-ultraviolet circular dichroism spectroscopy. Particular attention was paid to temperature-dependent structural changes. The results are discussed with reference to the native-like (N) state and the highly unfolded (U) state. It turned out that the I-state is most compact near 30 degrees C, having a Stokes radius 20% larger and a radius of gyration 30% larger than those of the N-state. Both cooling and heating relative to 30 degrees C led to an expansion of the molecule, but the structural changes at low and high temperatures were of a different kind. At temperatures above 40 degrees C non co-operative melting of structural elements was observed, while the secondary structure was essentially retained on cooling. The results are discussed in context with theoretical predictions of the compactness and the stability of apomyoglobin by Alonso et al. [Alonso, D. O. V., Dill, K. A., and Stigter, D. (1991) Biopolymers 31:1631-1649]. Comparing the I-state of apomyoglobin with the molten globules of alpha-lactalbumin and cytochrome c, we found that the compactness of the molten globule states of the three proteins decreases in the order alpha-lactalbumin > apocytochrome c > apomyoglobin.(ABSTRACT TRUNCATED AT 250 WORDS)

The temperature-dependent conformational equilibrium of 3-phosphoglycerate kinase has been studied in the temperature range from 1 to 30 degrees C by means of dynamic light scattering, small-angle X-ray scattering, differential scanning calorimetry, circular dichroism spectroscopy, and fluorescence spectroscopy. At 28 degrees C and in the presence of 0.7 M guanidine hydrochloride (GuHCl), the radius of gyration (RG) and the Stokes radius (RS) are 2.44 and 3.09 nm, respectively. Decreasing the temperature effects unfolding of the molecule, a process that involves two stages. The two stages correspond to the successive unfolding of the N-terminal and C-terminal domains. The peak maxima of the excess heat capacity, determined from differential calorimetric scans, extrapolated to 0 scan rate, are positioned at 16.5 degrees C for the N-terminal domain and at 6.3 degrees C for the C-terminal domain. At 4.5 degrees C, the radius of gyration and the Stokes radius increase to 7.8 and 4.8 nm, respectively. The persistence length and the length of the statistical chain segment of the unfolded polypeptide chain are 1.74 and 3.48 nm, corresponding to five and ten amino acids, respectively. At 1 degrees C, the dimensions of the unfolded chain nearly agree with the predicted dimensions under theta conditions. Thus, the conformational changes upon cold denaturation can be described by a transition from a compactly folded molecule to a random coil. The conformation-dependent ratio rho = RGRS-1 increases from rho = 0.79 to rho = 1.63. The volume of the unfolded chain is 30 times larger than that of the folded chain in the native state.(ABSTRACT TRUNCATED AT 250 WORDS)

The conformational transitions of bovine beta-lactoglobulin A and phosphoglycerate kinase from yeast induced by hexafluoroisopropanol (HFIP) and trifluoroethanol (TFE) have been studied by dynamic light scattering and circular dichroism spectroscopy in order to elucidate the potential of fluoroalcohols to bring about structural changes of proteins. Moreover, pure fluoroalcohol-water mixed solvents were investigated to prove the relation between cluster formation and the effects on proteins. The results demonstrate that cluster formation is mostly an accompanying phenomenon because important structural changes of the proteins occur well below the critical concentration of fluoroalcohol at which the formation of clusters sets in. According to our light scattering experiments, the remarkable potential of HFIP is a consequence of extensive preferential binding. Surprisingly, preferential binding seems to play a vanishing role in the case of TFE. However, the comparable Stokes radii of both proteins in the highly helical state induced by either HFIP or TFE point to a similar degree of solvation in both mixed solvents. This shows that direct binding or an indirect mechanism must be equally taken into consideration to explain the effects of alcohols on proteins. The existence of a compact helical intermediate with non-native secondary structure on the transition of beta-lactoglobulin A from the native to the highly helical state is clearly demonstrated.

Dynamic light scattering and circular dichroism experiments were performed to determine the compactness and residual secondary structure of reduced and by 6 M guanidine hydrochloride denatured ribonuclease A. We find that reduction of the four disulphide bonds by dithiothreitol at 20°C leads to total unfolding and that a temperature increase has no further effect on the dimension. The Stokes' radius of ribonuclease A at 20°C is R S = (1.90 4" 0.04) nm (native) and Rs = (3.14 4" 0.06) nm (reduced-denatured). Furthermore, circular dichroism spectra do not indicate any residual secondary structure. We suggest that reduced-denatured Ribonuclease A has a random coil-like conformation and is not in a compact denatured state.

The trifluoroethanol (TFE)-induced structural changes of two proteins widely used in folding experiments, bovine alpha-lactalbumin, and bovine pancreatic ribonuclease A, have been investigated. The experiments were performed using circular dichroism spectroscopy in the far- and near-UV region to monitor changes in the secondary and tertiary structures, respectively, and dynamic light scattering to measure the hydrodynamic dimensions and the intermolecular interactions of the proteins in different conformational states. Both proteins behave rather differently under the influence of TFE: alpha-lactalbumin exhibits a molten globule state at low TFE concentrations before it reaches the so-called TFE state, whereas ribonuclease A is directly transformed into the TFE state at TFE concentrations above 40% (v/v). The properties of the TFE-induced states are compared with those of equilibrium and kinetic intermediate states known from previous work to rationalize the use of TFE in yielding information about the folding of proteins. Additionally, we report on the properties of TFE/water and TFE/buffer mixtures derived from dynamic light scattering investigations under conditions used in our experiments.

During folding of globular proteins, the molten globule state was observed as an equilibrium intermediate under mildly denaturing conditions as well as a transient intermediate in kinetic refolding experiments. While the high compactness of the equilibrium intermediate of a-lactalbumin has been verified, direct measurements of the compactness of the kinetic intermediate have not been reported until now. Our dynamic light scattering measurements provide a complete set of the hydrodynamic dimensions of bovine a-lactalbumin in different conformational states, particularly in the kinetic molten globule state. The Stokes radii for the native, kinetic molten globule, equilibrium molten globule, and unfolded states are 1.9 1, I .99, 2.08, and 2.46 nm, respectively. Therefore, the kinetic intermediate appears to be even more compact than its equilibrium counterpart. Remarkable differences in the concentration dependence of the Stokes radius exist revealing strong attractive but repulsive intermolecular interactions in the kinetic and equilibrium molten globule states, respectively. This underlines the importance of extrapolation to zero protein concentration in measurements of the molecular compactness.