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. 2018 Mar 21;7:e34271. doi: 10.7554/eLife.34271

Table 1. Rates of transition between all observed FRET states for all three HIV-1 Envs.

The distribution of dwell times in each FRET state, determined through Hidden Markov Modeling (HMM), were fit to the sum of two exponential distributions (y = A1 exp k1t + A2 exp k2t) (Figure 4—figure supplements 13). The weighted average of the two rate constants from each fit are presented. Error bars represent 95% confidence intervals propagated from the kinetics analysis.

HIV-1NL4-3 k1→2 (s−1) k2→1 (s−1) k2→3 (s−1) k3→2 (s−1)
 Unliganded 1.50 ± 0.04 3.05 ± 0.04 1.89 ± 0.05 1.32 ± 0.04
 sCD4 2.10 ± 0.04 1.52 ± 0.04 1.21 ± 0.03 1.85 ± 0.03
 sCD4D1D2-Igαtp 1.60 ± 0.02 2.84 ± 0.04 1.87 ± 0.04 1.13 ± 0.02
HIV-1JR-FL
 Unliganded 1.30 ± 0.03 2.21 ± 0.03 1.70 ± 0.02 1.25 ± 0.02
 sCD4 1.52 ± 0.03 1.76 ± 0.04 2.25 ± 0.03 1.37 ± 0.05
 sCD4D1D2-Igαtp 2.02 ± 0.06 2.06 ± 0.05 1.81 ± 0.06 1.06 ± 0.03
HIV-1BG505
 Unliganded 1.10 ± 0.04 4.37 ± 0.08 2.86 ± 0.05 1.77 ± 0.03
 sCD4 1.21 ± 0.03 4.32 ± 0.08 1.81 ± 0.09 2.79 ± 0.04
 sCD4D1D2-Igαtp 1.62 ± 0.06 2.82 ± 0.05 2.92 ± 0.04 2.31 ± 0.05