Modulation of contact order effects in the two-state folding of stefins A and B.

It is well established that contact order and folding rates are correlated for small proteins. The folding rates of stefins A and B differ by nearly two orders of magnitude despite sharing an identical native fold and hence contact order. We break down the determinants of this behavior and demonstrate that the modulation of contact order effects can be accounted for by the combined contributions of a framework-like mechanism, characterized by intrinsic helix stabilities, together with nonnative helical backbone conformation and nonnative hydrophobic interactions within the folding transition state. These contributions result in the formation of nonnative interactions in the transition state as evidenced by the opposing effects on folding rate and stability of these proteins.

Directed evolution of a G protein-coupled receptor for expression, stability, and binding selectivity.

We outline a powerful method for the directed evolution of integral membrane proteins in the inner membrane of Escherichia coli. For a mammalian G protein-coupled receptor, we arrived at a sequence with an order-of-magnitude increase in functional expression that still retains the biochemical properties of wild type. This mutant also shows enhanced heterologous expression in eukaryotes (12-fold in Pichia pastoris and 3-fold in HEK293T cells) and greater stability when solubilized and purified, indicating that the biophysical properties of the protein had been under the pressure of selection. These improvements arise from multiple small contributions, which would be difficult to assemble by rational design. In a second screen, we rapidly pinpointed a single amino acid substitution in wild type that abolishes antagonist binding while retaining agonist-binding affinity. These approaches may alleviate existing bottlenecks in structural studies of these targets by providing sufficient quantities of stable variants in defined conformational states.

Essential role of proline isomerization in stefin B tetramer formation.

Here we present the tetrameric structure of stefin B, which is the result of a process by which two domain-swapped dimers of stefin B are transformed into tetramers. The transformation involves a previously unidentified process of extensive intermolecular contacts, termed hand shaking, which occurs concurrently with trans to cis isomerization of proline 74. This proline residue is widely conserved throughout the cystatin superfamily, a member of which, human cystatin C, is the key protein in cerebral amyloid angiopathy. These results are consistent with the hypothesis that isomerization of proline residues can play a decisive role in amyloidogenesis.

Folding and amyloid-fibril formation for a series of human stefins' chimeras: any correlation?

To study the influence of whole secondary structure elements to the process of folding and amyloid-fibril formation, chimeras of stefins have been prepared. GdnHCl denaturation curves and folding rates (chevron plots) have been analyzed based on a two-state mechanism. The order of stability is: stefin A > aAbbbb > bAbbbb > stefin B = aBaaaa > bBaaaa, where the make up of chimeric proteins is designated by small letters representing the source of individual strands (a for stefin A, b for stefin B) and a capital letter representing the source of the helix (A for stefin A and B for stefin B). Only the fast folding reactions were included in the analysis and it has been found that stefin B folds the fastest (657 s(-1)). Similarly, fast folders are the chimeric proteins aBaaaa and bBaaaa, both of which contain the alpha-helix of stefin B. Unfolding rates correlate very well with protein stability, with the slowest rate for the most stable protein, stefin A. Amyloid-fibril growth was measured for each protein by monitoring thioflavin T fluorescence and was visualized using electron microscopy. The propensity to form amyloid-fibrils is in the order: stefin B > bAbbbb > aAbbbb > bBaaaa > aBaaaa > stefin A. This order does not correlate with stability, or with the folding or unfolding rates. Instead, the propensity to fibrillize is related to selected parts of structure, such as the beta-sheet of stefin B, and can be predicted reasonably well by calculating the beta-strand propensity of the denatured states.

Differences in aggregation properties of three site-specific mutants of recombinant human stefin B.

We describe expression, purification, and characterization of three site-specific mutants of recombinant human stefin B: H75W, P36G, and P79S. The far- and near-UV CD spectra have shown that they have similar secondary and tertiary structures to the parent protein. The elution on gel-filtration suggests that recombinant human stefin B and the P36G variant are predominantly monomers, whereas the P79S variant is a dimer. ANS dye binding, reflecting exposed hydrophobic patches, is highest for the P36G variant, both at pH 5 and 3. ANS dye binding also is increased for stefin B and the other two variants at pH 3. Under the chosen conditions the highest tendency to form amyloid fibrils has been shown for the recombinant human stefin B. The P79S variant demonstrates a longer lag phase and a lower rate of fibril formation, while the P36G variant is most prone to amorphous aggregation. This was demonstrated by ThT fluorescence as a function of time and by transmission electron microscopy.

Different propensity to form amyloid fibrils by two homologous proteins-Human stefins A and B: searching for an explanation.

By using ThT fluorescence, X-ray diffraction, and atomic force microscopy (AFM), it has been shown that human stefins A and B (subfamily A of cystatins) form amyloid fibrils. Both protein fibrils show the 4.7 A and 10 A reflections characteristic for cross beta-structure. Similar height of approximately 3 nm and longitudinal repeat of 25-27 nm were observed by AFM for both protein fibrils. Fibrils with a double height of 5.6 nm were only observed with stefin A. The fibril's width for stefin A fibrils, as observed by transmission electron microscopy (TEM), was in the same range as previously reported for stefin B (Zerovnik et al., Biochem Biophys Acta 2002;1594:1-5). The conditions needed to undergo fibrillation differ, though. The amyloid fibrils start to form at pH 5 for stefin B, whereas in stefin A, preheated sample has to be acidified to pH < 2.5. In both cases, adding TFE, seeding, and alignment in a strong magnetic field accelerate the fibril growth. Visual analysis of the three-dimensional structures of monomers and domain-swapped dimers suggests that major differences in stability of both homologues stem from arrangement of specific salt bridges, which fix alpha-helix (and the alpha-loop) to beta-sheet in stefin A monomeric and dimeric forms.

Folding and unfolding mechanism of highly stable full-consensus ankyrin repeat proteins.

Full-consensus designed ankyrin repeat proteins were designed with one to six identical repeats flanked by capping repeats. These proteins express well in Escherichia coli as soluble monomers. Compared to our previously described designed ankyrin repeat protein library, randomized positions have now been fixed according to sequence statistics and structural considerations. Their stability increases with length and is even higher than that of library members, and those with more than three internal repeats are resistant to denaturation by boiling or guanidine hydrochloride. Full denaturation requires their heating in 5 M guanidine hydrochloride. The folding and unfolding kinetics of the proteins with up to three internal repeats were analyzed, as the other proteins could not be denatured. Folding is monophasic, with a rate that is nearly identical for all proteins ( approximately 400-800 s(-1)), indicating that essentially the same transition state must be crossed, possibly the folding of a single repeat. In contrast, the unfolding rate decreases by a factor of about 10(4) with increasing repeat number, directly reflecting thermodynamic stability in these extraordinarily slow denaturation rates. The number of unfolding phases also increases with repeat number. We analyzed the folding thermodynamics and kinetics both by classical two-state and three-state cooperative models and by an Ising-like model, where repeats are considered as two-state folding units that can be stabilized by interacting with their folded nearest neighbors. This Ising model globally describes both equilibrium and kinetic data very well and allows for a detailed explanation of the ankyrin repeat protein folding mechanism.