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Biophys J, August 2000, p. 934-944, Vol. 79, No. 2
-Peptide into Planar Bilayer Membranes

*Institute of Biomedical Sciences, Faculty of Medicine, University
of Chile, Santiago, Chile,
Laboratory of Biochemistry and
Cell Biology, National Institute of Diabetes and Digestive and Kidney
Diseases, National Institutes of Health, Bethesda, Maryland 20892 USA
and
Sansum Medical Research Institute, Santa Barbara, CA
93105 USA
The role of endogenous amyloid
-peptides as causal
factors of neurodegenerative diseases is largely unknown. We have
previously reported that interactions between Alzheimer's disease
A
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
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
P[1-40]-specific displacement currents, we added A
P[1-40] (1-5 µM) to the
solution on either side of the membrane and noted that the direction of the displacement current depended on the side with A
P[1-40]. The
size of the A
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
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 (Vo) were ~
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
P[1-40]-specific transfer of
charge reached a maximum value (Qmax) when
the electrical potential of the side containing the amyloid
-protein
was taken to either
300 or 300 mV. For a circular membrane of 25-µm
radius (~2000 µm2), the total A
P[1-40]-specific
charge Qmax was estimated as 55 fC,
corresponding to some 170 e.c./µm2. Regardless of
the side selected for the addition of A
P[1-40], at
Vo the charge displaced underwent an
e-fold change for a ~27-mV change in potential. The
effective valence (a) of the A
P[1-40] dipole
(i.e., the actual valence Z multiplied by the fraction of the electric field
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
P[40-1]). These data demonstrate that A
P[1-40] molecules can span the low dielectric domain of the bilayer, exposing charged residues (D1,
E3, R5, H6, D7,
E11, H13, and H14) to the electric
field. Thus the A
P[1-40] molecules in solution must spontaneously
acquire suitable conformations (
-pleated sheet) allowing specific
interactions with charged phospholipids. Interestingly, the domain from
residues 676 to 704 in the APP751 is homologous with the
consensus sequence for lipid binding found in other membrane proteins
regulated by anionic phospholipids.
Biophys J, August 2000, p. 934-944, Vol. 79, No. 2
© 2000 by the Biophysical Society 0006-3495/00/08/934/11 $2.00
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