Abstract
The reversibility of the binding of human apolipoprotein A-I (apo-A-I) to phospholipid was monitored through the influence of guanidine hydrochloride (Gdn.cntdot.HCl) on the isothermal denaturation and renaturation of apo A-I/dimyristoylphosphatidylcholine (DMPC) complexes at 24.degree. C. Denaturation was studied by incubating discoidal 1:100 and vesicular 1:500 mol/mol apo A-I/DMPC complexes with up to 7 M Gdn.cntdot.HCl for up to 72 h. Unfolding of apo-A-I molecules was observed from circular dichroism spectra while the distribution of protein between free and lipid-associated states was monitored by density gradient ultracentrifugation. The ability of apo A-I to combine with DMPC in the presence of Gdn.cntdot.HCl at 24.degree. C was also investigated by similar procedures. In both the denaturation and renaturation of 1:100 and 1:500 complexes, the final values of the molar ellipticity and the ratio of free to bound apo A-I at various concentrations of Gdn.cntdot.HCl are dependent on the initial state of the lipid and protein; apo A-I is more resistant to denaturation when Gdn.cntdot.HCl is added to existing complexes than to a mixture of apo A-I and DMPC. There is an intermediate state in the denaturation pathway of apo A-I/DMPC complexes which is not present in the renaturation; the intermediate comprises partially unfolded apo A-I molecules still associated with the complex by some of their apolar residues. Complete unfolding of the .alpha. helix and subsequent desorption of the apo A-I molecules from the lipid/water interface involve cooperative exposure of these apolar residues to the aqueous phase. The energy barrier associated with this desorption step makes the binding of apo A-I to DMPC a thermodynamically irreversible process. Consequently, binding constants of apo A-I and PC cannot be calculated simply from equilibrium thermodynamic treatments of the partitioning of protein between free and bound states. Apo A-I molecules do not exchange freely between the lipid-free and lipid-bound states, and extra work is required to drive protein molecules off the surface. The required increase in surface pressure can be achieved by a net mass transfer of protein to the surface; in vivo, increases in the surface pressure of lipoproteins by lipolysis can cause protein desorption.