Displacement currents associated with the insertion of Alzheimer disease amyloid beta-peptide into planar bilayer membranes.

The role of endogenous amyloid beta-peptides as causal factors of neurodegenerative diseases is largely unknown. We have previously reported that interactions between Alzheimer's disease A beta P[1-40] peptide in solution and planar bilayer membranes made from anionic phospholipids lead to the formation of cation-selective channels. We now find and report here that the spontaneous insertion of free A beta P[1-40] across the bilayer can be detected as an increase in bilayer capacity. To this end we recorded the displacement currents across planar bilayers (50 mM KCl on both sides) in response to sudden displacements of the membrane potential, from -300 to 300 mV in 20-mV increments. To monitor the A beta P[1-40]-specific displacement currents, we added A beta P[1-40] (1-5 microM) to the solution on either side of the membrane and noted that the direction of the displacement current depended on the side with A beta P[1-40]. The size of the A beta P[1-40]-specific charge displaced during a pulse was always equal to the charge returning to the original configuration after the pulse, suggesting that the dipole molecules are confined to the membrane. As a rule, the steady-state distribution of the A beta P[1-40]-specific charges within the bilayer could be fit by a Boltzmann distribution. The potential at which the charges were found to be equally distributed (V(o)) were approximately -135 mV (peptide added to the solution in the compartment electrically connected to earth) and 135 mV (peptide added to the solution connected to the input of the amplifier). The A beta P[1-40]-specific transfer of charge reached a maximum value (Q(max)) when the electrical potential of the side containing the amyloid beta-protein was taken to either -300 or 300 mV. For a circular membrane of 25-microm radius ( approximately 2000 microm(2)), the total A beta P[1-40]-specific charge Q(max) was estimated as 55 fC, corresponding to some 170 e.c./microm(2). Regardless of the side selected for the addition of A beta P[1-40], at V(o) the charge displaced underwent an e-fold change for a approximately 27-mV change in potential. The effective valence (a) of the A beta P[1-40] dipole (i.e., the actual valence Z multiplied by the fraction of the electric field chi acting on the dipole) varied from 1 to 2 electronic charges. We also tested, with negative results, the amyloid peptide with the reverse sequence (A beta P[40-1]). These data demonstrate that A beta P[1-40] molecules can span the low dielectric domain of the bilayer, exposing charged residues (D(1), E(3), R(5), H(6), D(7), E(11), H(13), and H(14)) to the electric field. Thus the A beta P[1-40] molecules in solution must spontaneously acquire suitable conformations (beta-pleated sheet) allowing specific interactions with charged phospholipids. Interestingly, the domain from residues 676 to 704 in the APP(751) is homologous with the consensus sequence for lipid binding found in other membrane proteins regulated by anionic phospholipids.