Journal of Molecular Biology
Membrane Fusogenic Activity of the Alzheimer's Peptide Aβ(1–42) Demonstrated by Small-Angle Neutron Scattering
Introduction
The emerging trend for the explanation of neurodegeneration in Alzheimer's disease (AD) imputes the cause of neurotoxicity to the interaction of soluble amyloid beta forms with neural cells.1 Amyloid-β peptides (Aβs) are peptides naturally found in the cerebrospinal liquids, and little is known about their physiological function. They are the product of the enzymatic cleavage of a longer transmembrane protein, the amyloid precursor protein, and they have been identified more than two decades ago as the principal component of the proteinaceous deposits characteristic of brain tissues of patients with AD.2 These so-called “senile plaques” primarily contain fibrils of Aβ, and it has been commonly believed that the Aβ fibrils were the toxic form of this peptide.3, 4, 5 More recently, it has been shown that soluble forms of Aβ cause neuronal dysfunction in vivo,6 and it was demonstrated that Aβ oligomers are more toxic than fibrils.7 In addition, it has been shown that Aβ(1–42) in the soluble form is nondetectable in plaque-free normal brain.8 Taken together, these experimental facts tend to identify the soluble and diffusible Aβ forms as the trigger of the neurodegenerative cascade of AD. Nevertheless, the mechanism of action of Aβ continues to remain unknown. The study of the interaction of Aβ with the neuronal membrane is a topic of great interest, in the attempt to identify whether the soluble amyloid beta binds to specific receptors or adsorbs nonspecifically to various receptors and channel proteins. In addition, there is evidence that Aβ and other amyloidogenic proteins can penetrate the membrane, leading to permeabilization and to pore formation.9 In our previous investigations, we had applied neutron diffraction and selective deuteration to localize the short peptide Aβ(25–35), a toxic fragment of Aβ, into lipid bilayers of different surface charge and composition.10, 11, 12 In the present study, the interaction of the most abundant Aβ in senile plaques, that is, Aβ(1–42), with unilamellar lipid vesicles (ULVs) is investigated by small-angle neutron scattering (SANS). SANS is a well-established technique for the investigation of lipid vesicles13 and the change of the parameters describing their structure in different conditions.14, 15, 16, 17 We have applied the recently proposed separated form factor (SFF) method18 to extruded unilamellar vesicles, and we have extracted the parameters characterizing the vesicle size, size distribution, and vesicle shell (i.e., lipid bilayer) by using different models to describe the bilayer profiles. The effect of Aβ on these parameters has been investigated as a function of pH and of Aβ concentration. The results clearly show the interaction of Aβ with respect to lipid membranes and allow assumptions about its localization in the bilayer.
Section snippets
Theory
SANS measurements from ULV contain different information about the vesicle structure in different regions of the scattering vector q. The low-q region (q < 0.02 Å–1) is affected by the vesicle shape and size and allows extracting the vesicle radius R and the polydispersivity. The high-q region (q > 0.1 Å–1) is modulated by the thickness of the shell d and is barely affected by vesicle radius and polydispersivity.
For monodisperse systems, the scattered intensity I(q) is given by:where
Results
We have investigated by SANS the interaction of monomeric and aged Aβ(1–42) with lipid vesicles.
The small-angle scattering curves obtained from the ULV dispersions at pD 7.0 and pD 6.0 at various Aβ(1–42) contents are shown in Fig. 3a and b. As thoroughly discussed elsewhere,25 the low-q region is influenced by the ULV form factor, while the scattering in the high-angle region is dominated by the form factor of the lipid bilayer. It is evident that the peptide affects the experimental curves
Discussion
In this article, the SFF method used to analyze and interpret small-angle scattering has been applied to curves obtained from ULV of phospholipids in the presence of different amounts of Aβ(1–42).
To our knowledge, although this method has already been proposed to investigate ULV of pure phospholipids, this is the first time that this method is employed to explain the change of the bilayer structure as a function of some physicochemical parameters. We have modified an existing fitting routine to
Sample preparation
POPC and the net negatively charged lipid POPS were purchased from Avanti Polar Lipids (Alabaster, AL) and used as received. The deuterated forms of these products, that is, POPC-D31 and POPS-D31, were also from Avanti Polar Lipids. Aβ(1–42) was a product of Bachem (Germany). D2O was a product of Sigma-Aldrich, and phosphate-buffered saline (PBS) was purchased from Fluka (Germany). The lipids were solubilized in 1:1 chloroform/methanol; the solvent was evaporated under a gentle stream of
Acknowledgements
The authors acknowledge Dr. Jeremy Pencer for kindly providing the fitting routine of the SANS data. This work was partially supported by the Deutsche Forschungsgemeinschaft (SFB 472).
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