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. 1998 May 26;95(11):6118-21.
doi: 10.1073/pnas.95.11.6118.

Huntingtin aggregation monitored by dynamic light scattering

Affiliations

Huntingtin aggregation monitored by dynamic light scattering

Y Georgalis et al. Proc Natl Acad Sci U S A. .

Abstract

An initial stage of fibrillogenesis in solutions of glutathione S-transferase-huntingtin (GST-HD) fusion proteins has been studied by using dynamic light scattering. Two GST-HD systems with poly-L-glutamine (polyGln) extensions of different lengths (20 and 51 residues) have been examined. For both systems, kinetics of z-average translation diffusion coefficients (Dapp) and their angular dependence have been obtained. Our data reveal that aggregation does occur in both GST-HD51 and GST-HD20 solutions, but that it is much more pronounced in the former. Thus, our approach provides a powerful tool for the quantitative assay of GST-HD fibrillogenesis in vitro.

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Figures

Figure 1
Figure 1
(A) Schematic representation of primary structure of GST-HD fusion proteins. The amino acid sequence corresponding to exon 1 of huntingtin is boxed. Q and P stand for polyglutamine and polyproline extensions, respectively. Arrows and T indicate cleavage sites for trypsin. (B) Site-specific proteolysis of GST-HD fusion proteins with trypsin. Tryptic digestions were performed at 37°C for the indicated times. Undigested and trypsin-digested proteins were subjected to 12.5% SDS/PAGE, blotted onto nitrocellulose membranes, and probed with the anti-huntingtin antibody HD1. Arrow marks the origin of electrophoresis.
Figure 2
Figure 2
(a) Apparent diffusion coefficient Dapp(t) plotted as function of time for selected fusion protein preparations GST-HD20 (•) and GST-HD51 (▪). Measurements were conducted at a fixed scattering angle, 45°. (b) Normalized second cumulant of GST-HD20 (•) and GST-HD51 (▪) as a function of time. Note that the 5-fold drop of the apparent diffusion coefficient is accompanied by a 100-fold increment of the normalized second cumulant, which can be understood as a drastic increment of the solution polydispersity.
Figure 3
Figure 3
Angular dependence of the z-average diffusion coefficient of the (a) GST-HD20 and (b) GST-HD51 protein preparations. SDs were estimated from an average of three experiments conducted 18 hr after collecting the time-resolved results shown in Fig. 2. Note that the q2 dependence of Dapp for both samples deviates appreciably from linearity. Further, the GST-HD20 sample exhibits roughly a two times higher limiting Dapp(q) value than the GST-HD51 one.
Figure 4
Figure 4
Electron micrographs of GST-HD20 (A and B) and GST-HD51 (C and D) proteins before (A and C) and after (B and D) treatment with trypsin. Samples were negatively stained with 1% uranyl acetate. (Scale bar = 100 nm.)

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