No abstract

The interaction of cytochrome c with anionic lipid vesicles of DOPS induces an extensive disruption of the native structure of the protein. The kinetics of this lipid-induced unfolding process were investigated in a series of fluorescence- and absorbance-detected stopped-flow measurements. The results show that the tightly packed native structure of cytochrome c is disrupted at a rate of ∼1.5 s-1 (independent of protein and lipid concentration), leading to the formation of a lipid-inserted denatured state (D L ). Comparison with the expected rate of unfolding in solution (∼2 × 10-3 s-1 at pH 5.0 in the absence of denaturant) suggests that the lipid environment dramatically accelerates the structural unfolding process of cytochrome c. We propose that this acceleration is in part due to the low effective pH in the vicinity of the lipid headgroups. This hypothesis was tested by comparative kinetic measurements of acid unfolding of cytochrome c in solution. Our absorbance and fluorescence kinetic data, combined with a well-characterized mechanism for folding/unfolding of cytochrome c in solution, allow us to propose a kinetic mechanism for cytochrome c unfolding at the membrane surface. Binding of native cytochrome c in water (N W ) to DOPS vesicles is driven by the electrostatic interaction between positively charged residues in the protein and the negatively charged lipid headgroups on the membrane surface. This binding step occurs within the dead time of the stopped-flow experiments (<2 ms), where a membrane-associated native state (N S ) is formed. Unfolding of N S driven by the acidic environment at the membrane surface is proposed to occur via a native-like intermediate lacking Met 80 ligation (M S ), as previously observed during unfolding in solution. The overall unfolding process (N S → D L ) is limited by the rate of disruption of the hydrophobic core in M S . Equilibrium spectroscopic measurements by near-IR and Soret absorbance, fluorescence, and circular dichroism showed that D L has native-like helical secondary structure, but shows no evidence for specific tertiary interactions. This lipid-denatured equilibrium state (D L ) is clearly more extensively unfolded than the A-state in solution, but is distinct from the unfolded protein in water (U W ), which has no stable secondary structure.

Although details of the molecular mechanisms for the uptake of the essential nutrient zinc into the bloodstream and its subsequent delivery to zinc-requiring organs and cells are poorly understood, it is clear that in vertebrates the majority of plasma zinc (9-14 microM; approx. 75-85%) is bound to serum albumin, constituting part of the so-called exchangeable pool. The binding of metal ions to serum albumins has been the subject of decades of studies, employing a multitude of techniques, but only recently has the identity and putative structure of the major zinc site on albumin been reported. Intriguingly, this site is located at the interface between two domains, and involves two residues from each of domains I and II. Comparisons of X-ray crystal structures of free and fatty-acid bound human serum albumin suggest that zinc binding to this site and fatty acid binding to one of the five major sites may be interdependent. Interactive binding of zinc and long-chain fatty acids to albumin may therefore have physiological implications.

Prion diseases are associated with a major refolding event of the normal cellular prion protein, PrP(C), where the predominantly alpha-helical and random coil structure of PrP(C) is converted into a beta-sheet-rich aggregated form, PrP(Sc). Under normal physiological conditions PrP(C) is attached to the outer leaflet of the plasma membrane via a GPI anchor, and it is plausible that an interaction between PrP and lipid membranes could be involved in the conversion of PrP(C) into PrP(Sc). Recombinant PrP can be refolded into an alpha-helical structure, designated alpha-PrP isoform, or into beta-sheet-rich states, designated beta-PrP isoform. The current study investigates the binding of beta-PrP to model lipid membranes and compares the structural changes in alpha- and beta-PrP induced upon membrane binding. beta-PrP binds to negatively charged POPG membranes and to raft membranes composed of DPPC, cholesterol, and sphingomyelin. Binding of beta-PrP to raft membranes results in substantial unfolding of beta-PrP. This membrane-associated largely unfolded state of PrP is slowly converted into fibrils. In contrast, beta-PrP and alpha-PrP gain structure with POPG membranes, which instead leads to amorphous aggregates. Furthermore, binding of beta-PrP to POPG has a disruptive effect on the integrity of the lipid bilayer, leading to total release of vesicle contents, whereas raft vesicles are not destabilized upon binding of beta-PrP.