Johan Leckner

The effect of the metal ion on the folding energetics of azurin: a comparison of the native, zinc and apoprotein.

The unfolding by guanidine hydrochloride (GuHCl) and the refolding on dilution of zinc and apoazurin have been monitored by far-UV circular dichroism (CD). With the native protein, the unfolding was followed by CD and optical absorption in the visible spectral region. With the zinc protein, the reversible unfolding has also been followed by tryptophan fluorescence and NMR. The zinc and Cu2+ metal ions remain associated with the protein in the unfolded state. When the unfolding of the native protein is followed by CD, the initial, reversible transition due to unfolding is followed by a slow change associated with the reduction of Cu2+ by the thiol group of the ligand Cys112. The unfolding of apoazurin displays two CD transitions, which evidence suggests represent different folding domains, the least stable one including the metal-binding site and the other one the rest of the beta-sheet structure. Both occur at a lower GuHCl concentration than the unfolding of the native protein. The CD titrations also demonstrate that zinc azurin has a lower stability than the copper protein. Unfolding of zinc azurin followed by tryptophan fluorescence occurs at a much lower GuHCl concentration than the CD changes, and NMR spectra show that there is no loss of secondary and tertiary structure at this concentration, whereas the CD-detected loss of secondary structure correlates with the NMR changes. Thus, the fluorescence change is ascribed to a small local perturbation of the structure around the single tryptophan residue. The differences in stability of the three forms of azurin are discussed in terms of the rack mechanism. A bound metal ion stabilizes the native fold, and this stabilization is larger for Cu(II) than for Zn(II), reflecting the higher affinity of the protein for Cu(II).

The effect of redox state on the folding free energy of azurin

Abstract The unfolding of oxidized and reduced azurin by guanidine hydrochloride has been monitored by circular dichroism. Dilution experiments showed the unfolding to be reversible, and the equilibrium data have been interpreted in terms of a two-state model. The protein is stabilized by the strong metal binding in the native state, so that the folding free energy is as high as –52.2 kJ mol–1 for the oxidized protein. The reduced protein is less stable, with a folding free energy of –40.0 kJ mol–1. A thermodynamic cycle shows, as a consequence, that unfolded azurin has a reduction potential 0.13 V above that of the folded protein. This is explained by the bipyramidal site in the native fold stabilizing Cu(II) by a rack mechanism, with the same geometry being maintained in the Cu(I) form. In the unfolded protein, on the other hand, the coordination geometries are expected to differ for the two oxidation states, Cu(I) being stabilized by the cysteine thiol group in a linear or trigonal symmetry, whereas Cu(II) prefers oxygen ligands in a tetragonal geometry.

Crystal structure of the disulfide bond-deficient azurin mutant C3A/C26A: how important is the S-S bond for folding and stability?

Azurin has a beta-barrel fold comprising eight beta-strands and one alpha helix. A disulfide bond between residues 3 and 26 connects the N-termini of beta strands beta1 and beta3. Three mutant proteins lacking the disulfide bond were constructed, C3A/C26A, C3A/C26I and a putative salt bridge (SB) in the C3A/S25R/C26A/K27R mutant. All three mutants exhibit spectroscopic properties similar to the wild-type protein. Furthermore, the crystal structure of the C3A/C26A mutant was determined at 2.0 A resolution and, in comparison to the wild-type protein, the only differences are found in the immediate proximity of the mutation. The mutants lose the 628 nm charge-transfer band at a temperature 10-22 degrees C lower than the wild-type protein. The folding of the zinc loaded C3A/C26A mutant was studied by guanidine hydrochloride (GdnHCl) induced denaturation monitored both by fluorescence and CD spectroscopy. The midpoint in the folding equilibrium, at 1.3 M GdnHCl, was observed using both CD and fluorescence spectroscopy. The free energy of folding determined from CD is -24.9 kJ.mol-1, a destabilization of approximately 20 kJ.mol-1 compared to the wild-type Zn2+-protein carrying an intact disulfide bond, indicating that the disulfide bond is important for giving azurin its stable structure. The C3A/C26I mutant is more stable and the SB mutant is less stable than C3A/C26A, both in terms of folding energy and thermal denaturation. The folding intermediate of the wild-type Zn2+-azurin is not observed for the disulfide-deficient C3A/C26A mutant. The rate of unfolding for the C3A/C26A mutant is similar to that of the wild-type protein, suggesting that the site of the mutation is not involved in an early unfolding reaction.

Apo-azurin folds via an intermediate that resembles the molten-globule.

The folding of Pseudomonas aeruginosa apo‐azurin was investigated with the intent of identifying putative intermediates. Two apo‐mutants were constructed by replacing the main metal‐binding ligand C112 with a serine (C112S) and an alanine (C112A). The guanidinium‐induced unfolding free energies (ΔGU−NH2O) of the C112S and C112A mutants were measured to 36.8 ± 1 kJ mole−1 and 26.1 ± 1 kJ mole−1, respectively, and the m‐value of the transition to 23.5 ± 0.7 kJ mole−1 M−1. The difference in folding free energy (ΔΔGU−NH2O) is largely attributed to the intramolecular hydrogen bonding properties of the serine Oγ in the C112S mutant, which is lacking in the C112A structure. Furthermore, only the unfolding rates differ between the two mutants, thus pointing to the energy of the native state as the source of the observed Δ ΔGU−NH2O. This also indicates that the formation of the hydrogen bonds present in C112S but absent in C112A is a late event in the folding of the apo‐protein, thus suggesting that formation of the metal‐binding site occurs after the rate‐limiting formation of the transition state. In both mutants we also noted a burst‐phase intermediate. Because this intermediate was capable of binding 1‐anilinonaphtalene‐8‐sulfonate (ANS), as were an acid‐induced species at pH 2.6, we ascribe it molten globule‐like status. However, despite the presence of an intermediate, the folding of apo‐azurin C112S is well approximated by a two‐state kinetic mechanism.

Probing the influence on folding behavior of structurally conserved core residues in P. aeruginosa apo-azurin

The effects on folding kinetics and equilibrium stability of core mutations in the apo‐mutant C112S of azurin from Pseudomonas aeruginosa were studied. A number of conserved residues within the cupredoxin family were recognized by sequential alignment as constituting a common hydrophobic core: I7, F15, L33, W48, F110, L50, V95, and V31. Of these, I7, V31, L33, and L50 were mutated for the purpose of obtaining information on the transition state and a potential folding nucleus. In addition, residue V5 in the immediate vicinity of the common core, as well as T52, separate from the core, were mutated as controls. All mutants exhibited a nonlinear dependence of activation free energy of folding on denaturant concentration, although the refolding kinetics of the V31A/C112S mutant indicated that the V31A mutation destabilizes the transition state enough to allow folding via a parallel transition state ensemble. Φ‐values could be calculated for three of the six mutants, V31A/C112S, L33A/C112S, and L50A/C112S, and the fractional values of 0.63, 0.33, and 0.50 (respectively) obtained at 0.5 M GdmCl suggest that these residues are important for stabilizing the transition state. Furthermore, a linear dependence of ln kobsH2O on ΔGU−NH2O of the core mutations and the putative involvement of ground‐state effects suggest the presence of native‐like residual interactions in the denatured state that bias this ensemble toward a folding‐competent state.