Table 1. Observed Aggregation Rates of α-Synuclein-A91C-Cy5 (500 nM), as a Function of the Amount of α-Synuclein-A91C-HTM on Beada.
Intercept
(AU) |
Slope (h–1) |
Statistics | |||
---|---|---|---|---|---|
αS-A91C-HTM | value | std er | value | std er | adj. R2 |
0 nM | 1.82 | 0.15 | 9.78 | 2.09 | 0.81 |
500 nM (no EtOH) | 1.85 | 0.34 | 6.01 | 1.11 | 0.85 |
500 nM | 2.19 | 0.36 | 326.94 | 17.56 | 0.99 |
250 nM | 2.06 | 0.18 | 221.31 | 8.74 | 0.99 |
100 nM | 2.45 | 0.07 | 149.22 | 2.74 | 1.00 |
50 nM | 2.31 | 0.08 | 67.24 | 1.68 | 1.00 |
25 nM | 2.34 | 0.07 | 51.07 | 1.16 | 1.00 |
Results from the fitting of the mean bead ring intensity in the Cy5 emission channel of data from Figure 4 for the different concentrations of α-synuclein-A91C-HTM incubated with the beads, using y = a + bx as a linear equation. At higher concentrations of α-synuclein-A91C-HTM, the slope of the fit increases, and the adjusted R2 decreases.