Ca(2+)- and H(+)-dependent conformational changes of calbindin D(28k).

Calbindin D(28k) is a member of a large family of intracellular Ca(2+) binding proteins characterized by EF-hand structural motifs. Some of these proteins are classified as Ca(2+)-sensor proteins, since they are involved in transducing intracellular Ca(2+) signals by exposing a hydrophobic patch on the protein surface in response to Ca(2+) binding. The hydrophobic patch serves as an interaction site for target enzymes. Other members of this group are classified as Ca(2+)-buffering proteins, because they remain closed after Ca(2+) binding and participate in Ca(2+) buffering and transport functions. ANS (8-anilinonaphthalene-1-sulfonic acid) binding and affinity chromatography on a hydrophobic column suggested that both the Ca(2+)-free and Ca(2+)-loaded form of calbindin D(28k) have exposed hydrophobic surfaces. Since exposure of hydrophobic surface is unfavorable in the aqueous intracellular milieu, calbindin D(28k) most likely interacts with other cellular components in vivo. A Ca(2+)-induced conformational change was readily detected by several optical spectroscopic methods. Thus, calbindin D(28k) shares some of the properties of Ca(2+)-sensor proteins. However, the Ca(2+)-induced change in exposed hydrophobic surface was considerably less pronounced than that in calmodulin. The data also shows that calbindin D(28k) undergoes a rapid and reversible conformational change in response to a H(+) concentration increase within the physiological pH range. The pH-dependent conformational change was shown to reside mainly in EF-hands 1-3. Urea-induced unfolding of the protein at pH 6, 7, and 8 showed that the stability of calbindin D(28k) was increased in response to H(+) in the range examined. The results suggest that calbindin D(28k) may interact with targets in a Ca(2+)- and H(+)-dependent manner.

Formation of short-lived protein aggregates directly from the coil in two-state folding.

Recent results on the 102 residue protein U1A show that protein aggregation is not always slow and irreversible but may take place transiently in refolding studies on a millisecond time scale. In this study we observe a similar aggregation behavior with the classical two-state protein CI2. Since both U1A and CI2 appear to fold directly from the coil at low protein concentrations, it is likely that the aggregates also form directly from the coil. This is in contrast to the behavior of larger multistate proteins where aggregation occurs in connection to "sticky" intermediates.

Alpha1-microglobulin chromophores are located to three lysine residues semiburied in the lipocalin pocket and associated with a novel lipophilic compound.

Alpha1-microglobulin (alpha1m) is an electrophoretically heterogeneous plasma protein. It belongs to the lipocalin superfamily, a group of proteins with a three-dimensional (3D) structure that forms an internal hydrophobic ligand-binding pocket. Alpha1m carries a covalently linked unidentified chromophore that gives the protein a characteristic brown color and extremely heterogeneous optical properties. Twenty-one different colored tryptic peptides corresponding to residues 88-94, 118-121, and 122-134 of human alpha1m were purified. In these peptides, the side chains of Lys92, Lys118, and Lys130 carried size heterogeneous, covalently attached, unidentified chromophores with molecular masses between 122 and 282 atomic mass units (amu). In addition, a previously unknown uncolored lipophilic 282 amu compound was found strongly, but noncovalently associated with the colored peptides. Uncolored tryptic peptides containing the same Lys residues were also purified. These peptides did not carry any additional mass (i.e., chromophore) suggesting that only a fraction of the Lys92, Lys118, and Lys130 are modified. The results can explain the size, charge, and optical heterogeneity of alpha1m. A 3D model of alpha1m, based on the structure of rat epididymal retinoic acid-binding protein (ERABP), suggests that Lys92, Lys118, and Lys130 are semiburied near the entrance of the lipocalin pocket. This was supported by the fluorescence spectra of alpha1m under native and denatured conditions, which indicated that the chromophores are buried, or semiburied, in the interior of the protein. In human plasma, approximately 50% of alpha1m is complex bound to IgA. Only the free alpha1m carried colored groups, whereas alpha1m linked to IgA was uncolored.

The changing nature of the protein folding transition state: implications for the shape of the free-energy profile for folding.

According to landscape theory proteins do not fold by localised pathways, but find their native conformation by a progressive organisation of an ensemble of partly folded structures down a folding funnel. Here, we use kinetics and protein engineering to investigate the shape of the free-energy profile for two-state folding, which is the macroscopic view of the funnel process for small and rapidly folding proteins. Our experiments are based mainly on structural changes of the transition state of chymotrypsin inhibitor 2 (CI2) upon destabilisation with temperature and GdnHCl. The transition state ensemble of CI2 is a localised feature in the free-energy profile that is sharply higher than the other parts of the activation barrier. The relatively fixed position of the CI2 transition state on the reaction coordinate makes it easy to characterise but contributes also to overshadow the rest of the free-energy profile, the shape of which is inaccessible for analysis. Results from mutants of CI2 and comparison with other two-state proteins, however, point at the possibility that the barrier for folding is generally broad and that localised transition states result from minor ripples in the free-energy profile. Accordingly, variabilities in the folding kinetics may not indicate different folding mechanisms, but could be accounted for by various degrees of ruggedness on top of very broad activation barriers for folding. The concept is attractive since it summarises a wide range of folding data which have previously seemed unrelated. It is also supported by theory. Consistent with experiment, broad barriers predict that new transition state ensembles are exposed upon extreme destabilisation or radical mutations.

High-energy channeling in protein folding.

Recent controversy about the role of populated intermediates in protein folding emphasizes the need to better characterize other events on the folding pathway. A complication is that these involve high-energy states which are difficult to target experimentally since they do not accumulate kinetically. Here, we explore the energetics of high-energy states and map out the shape of the free-energy profile for folding of the two-state protein U1A. The analysis is based on nonlinearities in the GdnHCl dependence of the activation energy for unfolding, which we interpret in terms of structural changes of the protein-folding transition state. The result suggests that U1A folds by high-energy channeling where most of the conformational search takes place isoenergetically at transition-state level. This is manifested in a very broad and flat activation barrier, the top of which covers more than 60% of the reaction coordinate. The interpretation favors a folding mechanism where the pathway leading to the native protein is determined by the sequence's ability to stabilize productive transition states.

Transient aggregates in protein folding are easily mistaken for folding intermediates.

It has been questioned recently whether populated intermediates are important for the protein folding process or are artefacts trapped in nonproductive pathways. We report here that the rapidly formed intermediate of the spliceosomal protein U1A is an off-pathway artefact caused by transient aggregation of denatured protein under native conditions. Transient aggregates are easily mistaken for structured monomers and could be a general problem in time-resolved folding studies.