Calorimetric determination of the energetics of the molten globule intermediate in protein folding: apo-.alpha.-lactalbumin

Volumetric Characterizations of the Native, Molten Globule and Unfolded States of Cytochrome cat Acidic pH

All-or-none solvent-induced transitions between native, molten globule and unfolded states in globular proteins

Comparison of the Conformational Stability of the Molten Globule and Native States of Horse Cytochrome c: Effects of Acetylation, Heat, Urea and Guanidine-Hydrochloride

We have investigated the thermal unfolding of bovine alpha-lactalbumin by means of circular dichroism spectroscopy in the far- and near-ultraviolet regions, and shown that the native alpha-lactalbumin undergoes heat and cold denaturation. The guanidine hydrochloride-induced unfolding of alpha-lactalbumin was also investigated by circular dichroism spectroscopy at various temperatures from 261 to 318 K. It is shown that the population of the molten globule state is strongly dependent on temperature and that the molten globule state does not accumulate during the guanidine hydrochloride-induced unfolding transition at 261 K. Our results indicate that the molten globule state of alpha-lactalbumin undergoes cold denaturation as the native alpha-lactalbumin does, and that the heat capacity change of unfolding from the molten globule to the unfolded state is positive and significant. The present results further support the idea that the molten globule and the unfolded states do not belong to the same thermodynamic state, and that the native, molten globule and unfolded states are sufficient for interpreting the guanidine hydrochloride-induced unfolding behavior of alpha-lactalbumin.

An intensively investigated intermediate state of protein folding is the molten globule (MG) state, which contains secondary but hardly any tertiary structure. In previous work, we have determined the distances between interacting spins within maltose binding protein (MBP) in its native state using continuous wave and double electron-electron resonance (DEER) electron paramagnetic resonance (EPR) spectroscopy. Seven double mutants had been employed to investigate the structure within the two domains of MBP. DEER data nicely corroborated the previously available X-ray data. Even in its MG state, MBP is known to still bind its ligand maltose. We therefore hypothesized that there must be a defined structure around the binding pocket of MBP already in the absence of tertiary structure. Here we have investigated the functional and structural difference between native and MG state in the open and closed form with a new set of MBP mutants. In these, the spin-label positions were placed near the active site. Binding of its ligands leads to a conformational change from open to closed state, where the two domains are more closely together. The complete set of MBP mutants was analyzed at pH 3.2 (MG) and pH 7.4 (native state) using double-quantum coherence EPR. The values were compared with theoretical predictions of distances between the labels in biradicals constructed by molecular modeling from the crystal structures of MBP in open and closed form and were found to be in excellent agreement. Measurements show a defined structure around the binding pocket of MBP in MG, which explains maltose binding. A new and important finding is that in both states ligand-free MBP can be found in open and closed form, while ligand-bound MBP appears only in closed form because of maltose binding.

The fluorescence properties of three variants of alpha-lactalbumin (alpha-LA) containing a single tryptophan residue were investigated under native, molten globule, and unfolded conditions. These proteins have levels of secondary structure and stability similar to those of the wild type. The fluorescence signal in the native state is dominated by that of W104, with the signal of W60 and W118 significantly quenched by the disulfide bonds in their vicinity. In the molten globule state, the magnitude of the fluorescence signal of W60 and W118 increases, due to the loss of rigid, specific side chain packing. In contrast, the magnitude of the signal of W104 decreases in the molten globule state, perhaps due to the protonation of H107 or quenching by D102 or K108. The solvent accessibilities of individual tryptophan residues were investigated by their fluorescence emission maximum and by acrylamide quenching studies. In the native state, the order of solvent accessibility is as follows: W118 > W60 > W104. This order changes to W60 > W104 > W118 in the molten globule state. Remarkably, the solvent accessibility of W118 in the alpha-LA molten globule is lower than that in the native state. The dynamic properties of the three tryptophan residues were examined by time-resolved fluorescence anisotropy decay studies. The overall rotation of the molecule can be observed in both the native and molten globule states. In the molten globule state, there is an increase in the extent of local backbone fluctuations with respect to the native state. However, the fluctuation is not sufficient to result in complete motional averaging. The three tryptophan residues in the native and molten globule states have different degrees of motional freedom, reflecting the folding pattern and dynamic heterogeneity of these states. Taken together, these studies provide new insight into the structure and dynamics of the alpha-LA molten globule, which serves as a prototype for partially folded proteins.

The structure, stability, and unfolding-refolding kinetics of a chimeric protein, in which the amino acid sequence of the flexible loop region (residues 105-110) comes from equine lysozyme and the remainder of the sequence comes from bovine alpha-lactalbumin were studied by circular dichroism spectroscopy and stopped-flow measurements, and the results were compared with those of bovine alpha-lactalbumin. The substitution of the flexible loop in bovine alpha-lactalbumin with the helix D of equine lysozyme destabilizes the molten globule state, although the native state is significantly stabilized by substitution of the flexible loop region. The kinetic refolding and unfolding experiments showed that the chimeric protein refolds significantly faster and unfolds substantially slower than bovine alpha-lactalbumin. To characterize the transition state between the molten globule and the native states, we investigated the guanidine hydrochloride concentration dependence of the rate constants of refolding and unfolding. Despite the significant differences in the stabilities of both the molten globule and native states between the chimeric protein and bovine alpha-lactalbumin, the free energy level of the transition state is not affected by the amino acid substitution in the flexible loop region. Our results suggest that the destabilization in the molten globule state of the chimeric protein is caused by the disruption of the non-native interaction in the flexible loop region and that the disruption of the non-native interaction reduces the free energy barrier of refolding. We conclude that the non-native interaction in the molten globule state may act as a kinetic trap for the folding of alpha-lactalbumin.

Equilibrium and kinetics of the folding of equine lysozyme studied by circular dichroism spectroscopy

The interaction of nile red (NR) with apomyoglobin (ApoMb) in the native (pH 7) and molten globule (pH 4) states was investigated using experimental and computational methods. NR binds to hydrophobic locations in ApoMb with higher affinity (K(d) = 25 +/- 5 microM) in the native state than in the molten globule state (K(d) = 52 +/- 5 microM). In the molten globule state, NR is located in a more hydrophobic environment. The dye does not bind to the holoprotein, suggesting that the binding site is located at the heme pocket. In addition to monitoring steady-state properties, the fluorescence emission of NR is capable of tracking submillisecond, time-resolved structural rearrangements of the protein, induced by a nanosecond pH jump. Molecular dynamics simulations were run on ApoMb at neutral pH and at pH 4. The structure obtained for the molten globule state is consistent with the experimentally available structural data. The docking of NR with the crystal structure shows that the ligand binds into the binding pocket of the heme group, with an orientation bringing the planar ring system of NR to overlap with the position of two of the heme porphyrin rings in Mb. The docking of NR with the ApoMb structure at pH 4 shows that the dye binds to the heme pocket with a slightly less favorable binding energy, in keeping with the experimental K(d) value. Under these conditions, NR is positioned in a different orientation, reaching a more hydrophobic environment in agreement with the spectroscopic data.

The acid-induced unfolding of myoglobin and its haem-free derivative apo-myoglobin is studied by broadband dielectric relaxation spectroscopy at pH values near 5, 4 and 2, which reflect the transition N → MG → UA from the native state (N) via a molten globule state (MG) to an acid-unfolded state (UA). Spectral changes are singled out by considering difference spectra for the transitions N → MG and N → UA. A pronounced increase of the amplitude of the tumbling motion of holo-myoglobin and apo-myoglobin in the sequence N → MG→ UA reflects the increase of their electrical dipole moments by progressive unfolding. A distinct high-frequency shoulder of the tumbling mode indicates an enhanced internal protein dynamics in the unfolded states. The calculated Stokes radii confirm a compact nature of the MG state and a large increase in size of the UA state relative to the native state. In the native state the Stokes radii deduced from the dielectric spectra agree fairly well with those deduced from dynamic light scattering. In the MG state, and particularly in the UA state, the Stokes radii determined by light scattering are markedly larger than those determined by dielectric relaxation. The difference is attributed to aggregation of the unfolded species, which affects dynamic light scattering more than dielectric relaxation. In the high-frequency regime, the dielectric spectra indicate that unfolding enhances the number of water molecules showing bulk-like dynamics, but the effect is rather weak.

The unfolding pathways of the native and molten globule states of 5-aminolevulinate synthase

The direct energy transfer technique was modified and applied to probe the relative localization of apomyoglobin A-, G- and H-helixes, which are partly protected from deuterium exchange in the equilibrium molten globule state and in the molten globule-like kinetic intermediate. The non-radiative transfer of tryptophan electronic energy to 3-nitrotyrosine was studied in different conformational states of apomyoglobin (native, molten globule, unfolded) and interpreted in terms of average distances between groups of the protein chain. The experimental data show that the distance between the middle of A-helix and the N-terminus of G-helix as well as the distance between the middle of the A-helix and the C-terminus of the H-helix in the molten globule state are close to those in the native state. This is a strong argument in favor of similarity of the overall architecture of the molten globule and native states.

The molten globule is a third thermodynamical state of protein molecules

The equilibrium and kinetics of the unfolding and refolding of authentic and recombinant human alpha-lactalbumin, the latter of which had an extra methionine residue at the N-terminus, were studied by circular dichroism spectroscopy, and the results were compared with the results for bovine and goat alpha-lactalbumins obtained in our previous studies. As observed in the bovine and goat proteins, the presence of the extra methionine residue in the recombinant protein remarkably destabilized the native state, and the destabilization was entirely ascribed to an increase in the rate of unfolding. The thermodynamic stability of the native state against the unfolded state was lower, and the thermodynamic stability of the molten globule state against the unfolded state was higher for the human protein than for the other alpha-lactalbumins previously studied. Thus, the population of the molten globule intermediate was higher during the equilibrium unfolding of human alpha-lactalbumin by guanidine hydrochloride. Unlike the molten globule states of the bovine and goat proteins, the human alpha-lactalbumin molten globule showed remarkably more intense circular dichroism ellipticity than the native state in the far-ultraviolet region below 225 nm. During refolding from the unfolded state, human alpha-lactalbumin thus exhibited overshoot kinetics, in which the alpha-helical peptide ellipticity exceeded the native value when the molten globule folding intermediate was formed in the burst phase. The subsequent folding involved reorganization of nonnative secondary structures. It should be noted that the rate constant of the major refolding phase was approximately the same among the three types of alpha-lactalbumin and that the rate constant of unfolding was accelerated 18-600 times in the human protein, and these results interpreted the lower thermodynamic stability of this protein.

Recent experiments have shown that the time dependence of fluorescence Stokes shift of a chromophore is substantially different when the chromophore is located in a molten globule (MG) state and in the native state of the same protein. To understand the origin of this difference, particularly the role of water in the differential solvation of the protein in the native and the MG states, we have carried out fully atomistic molecular dynamics simulations with explicit water of a partially unfolded MG state of the protein HP-36 and compared the results with the solvation dynamics of the protein in the folded native state. It is observed that the polar solvation dynamics of the three helical segments of the protein is influenced in a nonuniform heterogeneous manner in the MG state. While the equilibrium solvation time correlation function for helix-3 has been found to relax faster in the MG state as compared to that in the native state, the decay of the corresponding function for the other two helices slows down in the MG state. A careful analysis shows that the origin of such heterogeneous relative solvation behavior lies in the differential location of the polar probe residues and their exposure to bulk solvent. We find a significant negative cross-correlation between the contribution (to the solvation energy of a tagged amino acid residue) of water and the other groups of the protein, indicating a competing role in solvation. The sensitivity of solvation dynamics to the secondary structure and the immediate environment can be used to discriminate the partially unfolded and folded states. These results therefore should be useful in explaining recent solvation dynamics experiments on native and MG states of proteins.