| Literature DB >> 33810433 |
Agnes Paulus1,2, Anders Engdahl1, Yiyi Yang2, Antonio Boza-Serrano2, Sara Bachiller2, Laura Torres-Garcia3,4, Alexander Svanbergsson4, Megg G Garcia2,3, Gunnar K Gouras3, Jia-Yi Li4, Tomas Deierborg2, Oxana Klementieva1,5.
Abstract
Alzheimer's disease affects millions of lives worldwide. This terminal disease is characterized by the formation of amyloid aggregates, so-called amyloid oligomers. These oligomers are composed of β-sheet structures, which are believed to be neurotoxic. However, the actual secondary structure that contributes most to neurotoxicity remains unknown. This lack of knowledge is due to the challenging nature of characterizing the secondary structure of amyloids in cells. To overcome this and investigate the molecular changes in proteins directly in cells, we used synchrotron-based infrared microspectroscopy, a label-free and non-destructive technique available for in situ molecular imaging, to detect structural changes in proteins and lipids. Specifically, we evaluated the formation of β-sheet structures in different monogenic and bigenic cellular models of Alzheimer's disease that we generated for this study. We report on the possibility to discern different amyloid signatures directly in cells using infrared microspectroscopy and demonstrate that bigenic (amyloid-β, α-synuclein) and (amyloid-β, Tau) neuron-like cells display changes in β-sheet load. Altogether, our findings support the notion that different molecular mechanisms of amyloid aggregation, as opposed to a common mechanism, are triggered by the specific cellular environment and, therefore, that various mechanisms lead to the development of Alzheimer's disease.Entities:
Keywords: Alzheimer’s disease; FTIR; Tau; amyloid-β; cellular environment; α-synuclein β-sheet
Year: 2021 PMID: 33810433 PMCID: PMC8037084 DOI: 10.3390/ijms22073430
Source DB: PubMed Journal: Int J Mol Sci ISSN: 1422-0067 Impact factor: 5.923
Figure 1Immunofluorescent characterization of Aβ in cellular models of Alzheimer’s disease (AD). (A) Immunofluorescent labeling of Aβ with 82E1 (red) and amyloid fibrils with OC78 (white). The green fluorescence channel corresponds to mutated Tau (P301L) or αSyn (A53T) coupled to GFP. Bright-field images show the condition of fluorescence-activated cell sorting (FACS)-sorted cells (Supplementary Figures S2–S5). The scale bar is 20 µm. (B) Quantification of particle size was calculated using surface areas in immunosignal corresponding to 82E1 immunoreactivity. Aggregated Aβ was computed by co-localization analysis of Aβ (82E1) and amyloid fibrils (OC78). A threshold was set at 5% of max size (Supplementary Figure S6). (C) Statistical analysis of the co-localization of Aβ with fibrillary Aβ: one-way ANOVA (p < 0.01) ± s.d; n = 25–35 cells per sample. A coefficient of 1 is equal to 100% co-localization.
Summary of peak positions used in the study.
| Wavenumbers (cm−1) | Structure |
|---|---|
| 1656 cm−1 | C=O stretching, Amide I |
| 1550 cm−1 | C–N stretching; N–H bending, Amide II |
| 1628 cm−1 | β-sheet (main) |
| 1640 cm−1 | random coils (unordered) |
| 1656 cm−1 | α-helix |
| 1691 cm−1 | β-sheet (weak) |
| 1740 cm−1 | C=O bond of the ester peak |
Summary of bands ratios used for infrared spectra analysis.
| Ratio | Structure |
|---|---|
| 1550 cm−1/1656 cm−1 | protein folding |
| 1628 cm−1/1656 cm−1 | parallel β-sheet features |
| 1640 cm−1/1656 cm−1 | random coils (unordered) |
| 1691 cm−1/1628 cm−1 | anti-parallel β-sheet |
| 1740 cm−1/1656 cm−1 | C=O, lipid oxidation |
Figure 2Effect of αSyn (A53T) on Aβ aggregation in Aβ/αSyn cellular model of AD. (A) Averaged and normalized infrared absorbance spectra and corresponding normalized second derivatives of N2a-APPSWE, N2a-αSyn, N2a-APPSWE-αSyn. Dashed lines indicate peak positions. (B) Statistical analysis of structural changes. One-way ANOVA (p < 0.01) ± s.d; one dot corresponds to a single cell; n = 7–20 cells per independent measurement reproduced at least twice. All values are normalized to the control—N2a-APPSWE cells. (C) Averaged and normalized infrared absorbance spectra of N2a-APPSWE and N2a cells untransfected (left panel) and transfected with GFP (right panel).
Figure 3Effect of Tau (P301L) on Aβ aggregation in Aβ/Tau cellular model of AD. (A) Averaged and normalized infrared absorbance spectra and corresponding normalized second derivatives of N2a-APPSWE, N2a-Tau, N2a-APPSWE-Tau. Dashed lines indicate peak positions (B) Statistical analysis of structural changes. One-way ANOVA (p < 0.01) ± s.d; one dot corresponds to a single cell, n = 7–20 cells per independent measurement, reproduced at least twice. All values were normalized to the control—N2a-APPSWE cells.
Figure 4Comparison of structural changes in protein aggregates in the monogenic models of protein aggregation related to AD. (A) Averaged and normalized infrared absorbance spectra and corresponding normalized second derivatives of N2a-APPSWE, N2a-αSyn, N2a-Tau. Numbers in parenthesis indicate corresponding graphs with statistical analysis. Dashed lines indicate peak positions. (B) Statistical analysis of structural changes: one-way ANOVA (p < 0.01) ± s.d. All values were normalized to the control, N2a-APPSWE cells. One dot corresponds to a single cell, n = 7–20 cells per independent measurement reproduced at least twice.
Figure 5Comparison of structural changes in protein aggregates in the bigenic models of AD protein aggregation. (A) Averaged and normalized infrared absorbance spectra and corresponding normalized second derivatives of N2a-APPSWE, N2a-APPSWE-αSyn, and N2a-APPSWE-Tau, models of mixed protein aggregation. Numbers in parentheses indicate corresponding graphs with statistical analysis. Dashed lines indicate peak positions. (B) Statistical analysis of structural changes: one-way ANOVA (p < 0.01) ± s.d. All values were normalized to the control, N2a-APPSWE cells. One dot corresponds to a single cell, n = 7–20 cells per independent measurement reproduced at least twice.